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  <front>
    <journal-meta><journal-id journal-id-type="publisher">HGSS</journal-id><journal-title-group>
    <journal-title>History of Geo- and Space Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">HGSS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Hist. Geo Space. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2190-5029</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/hgss-13-1-2022</article-id><title-group><article-title>History of EISCAT – Part 5: Operation and development of the system during
the first 2 decades</article-title><alt-title>History of EISCAT</alt-title>
      </title-group><?xmltex \runningtitle{History of EISCAT}?><?xmltex \runningauthor{G.~Wannberg}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes">
          <name><surname>Wannberg</surname><given-names>Gudmund</given-names></name>
          <email>gudmund@wannbergradar.se</email>
        </contrib>
        <aff id="aff1"><institution>Wannberg radarkonsult AB,
Östra Trösten 141, 82951 Bergsjö, Sweden</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Gudmund Wannberg (gudmund@wannbergradar.se)</corresp></author-notes><pub-date><day>31</day><month>January</month><year>2022</year></pub-date>
      
      <volume>13</volume>
      <issue>1</issue>
      <fpage>1</fpage><lpage>21</lpage>
      <history>
        <date date-type="received"><day>17</day><month>September</month><year>2021</year></date>
           <date date-type="rev-request"><day>30</day><month>September</month><year>2021</year></date>
           <date date-type="rev-recd"><day>16</day><month>December</month><year>2021</year></date>
           <date date-type="accepted"><day>22</day><month>December</month><year>2021</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Gudmund Wannberg</copyright-statement>
        <copyright-year>2022</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://hgss.copernicus.org/articles/13/1/2022/hgss-13-1-2022.html">This article is available from https://hgss.copernicus.org/articles/13/1/2022/hgss-13-1-2022.html</self-uri><self-uri xlink:href="https://hgss.copernicus.org/articles/13/1/2022/hgss-13-1-2022.pdf">The full text article is available as a PDF file from https://hgss.copernicus.org/articles/13/1/2022/hgss-13-1-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e78">This paper gives an inside view of the first 20 years of operation of the
Kiruna–Sodankylä–Tromsø (KST) part of EISCAT as experienced and
remembered by myself. The paper is subdivided into an Introduction and 14 additional sections. Sections 2 to 7 describe the organisation, staffing and
responsibilities of the sites, with particular emphasis on the
transmitter-related work at Tromsø and the commuting of staff and
equipment between the sites. The headquarters operation is treated in
Sect. 8. The UHF radar system is treated in Sect. 9. Section 10 is a
review of the VHF system, including a summary of transmitter and antenna
problems not available elsewhere in easily accessed media. Section 11 treats
the computer system and the proprietary control languages EROS, TARLAN and
CORLAN. Section 12 describes the signal processing hardware, with special
emphasis on the Alker correlator, its idiosyncrasies and the gradual
unlocking of its capabilities through UNIPROG, the GEN system and the
G2 system, culminating in the ability to run alternating code experiments
routinely. Section 13 presents the time and frequency keeping, a
non-trivial task in the early 1980s. Finally, Sect. 14 discusses the UHF
spectrum problem and relates how the UHF system had to be constantly
upgraded in order to be able to co-exist with the emerging mobile phone
networks until the final closure of UHF reception at Kiruna and
Sodankylä in 2012. The paper ends with some personal reflections
(Sect. 15).</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e90">EISCAT, the European Incoherent SCATter radar system, is a multi-site
incoherent scatter radar (ISR) system, originally planned for studies of the auroral ionosphere and
located in the auroral zone in northern Finland, Norway and Sweden. Thanks
to its ability to provide spatially and temporally resolved measurements of
plasma parameters (plasma density, ion and electron temperatures, ion mass
and bulk velocities) throughout the ionosphere, from the D layer to the
topside, incoherent scatter is a powerful ground-based tool for ionosphere
and upper atmosphere studies.</p>
      <p id="d1e93">EISCAT was conceived in the late 1960s by a group of Nordic ionospheric
physicists, who managed to win URSI support for the concept at the 1969 URSI
General Assembly. Scientists from France, Germany and the United Kingdom
then joined the initiators, the movement eventually leading to the
establishment of the EISCAT Scientific Association. Important lessons from
an already operating incoherent radar system, personal memories of the
formation process, the financing negotiations and the subsequent design and
construction of the three “mainland” radar stations have been published in
previous papers of the present series (see references below).</p>
      <p id="d1e96">In retrospect, it is clear that the EISCAT system was established at the
best possible time, when there was a brief window of opportunity where
all the technical prerequisites for wideband incoherent scatter studies of
the ionosphere were on hand at the same time.</p>
      <p id="d1e99">In the early 1970s, blocks of unused and partially unallocated VHF and UHF
spectrum in the frequency ranges optimal for ionospheric incoherent scatter
observations and wide enough to receive the full scatter spectrum (10–15 MHz) were still available in the Nordic countries. Also, the theory of
incoherent scatter was well established, several ISR installations had been
working for a number of years, and high-power UHF and VHF radar technology, a
product of<?pagebreak page2?> the 1950s nuclear craze, had been developed to the point where
pulsed multi-megawatt transmitters could be had from industry. Low-noise UHF
receivers had become commercially available, the emerging satellite
communications industry had prompted the development of standardised
reflector antennas in the 32 m class, digital signal processing tools
capable of doing full justice to wideband incoherent scatter signals were
coming on line and their performance was increasing by orders of magnitude
every few years – so the technology was there, albeit large, costly and
partly clumsy. Last but not least, the number of sensitive electronic
devices in ordinary households was very small or non-existent, so the risk of
a radar system established in a populated environment generating
interference to consumer equipment was negligible.</p>
      <p id="d1e103">Over its more than 40 years of active operation, the EISCAT system has
generated a vast amount of groundbreaking ionospheric, magnetospheric and
middle atmosphere science. Starting from the “Green Book”  list of key
scientific questions, the so-called “eleven wonders of EISCAT” (du Castel
et al., 1971), the research has taken off in many different directions, some
aiming at investigating pre-existing hypotheses and models of the ionosphere
and thermosphere, others looking for rare and hard to detect plasma
conditions and processes, and yet others following up the surprising number
of observations of phenomena and processes not considered in the planning
stage, such as VHF and UHF polar
mesospheric summer echoes (PMSEs; e.g. Röttger et al., 1988),
non-equilibrium plasma processes at F region altitudes (e.g. Lockwood et
al., 1988), meteor head echoes and different kinds of coherent echoes.</p>
      <p id="d1e106">This work has been extensively reported in a large number of peer-reviewed
papers, conference proceedings and internal reports; according to the
statistics kept by EISCAT headquarters, the total number of publications now
exceeds 2500! It is beyond the capability of a single historical paper to
give due credit to all this work; it stands solidly on its own merits.</p>
      <p id="d1e109">However, the first step towards all these achievements has been the
generation, recording and distribution of raw radar data and in many cases
also the analysis of the data into physical parameters. This work has been
the responsibility of the EISCAT staff. It may not be very visible to the
typical data user, but nevertheless all important to the overall mission. I
was part of this work from 1981 to 2008, and probably because of this long
history, I have been asked to share my memories of what life at EISCAT was
like during the first 2 decades. In the following, I try to give my
insider's view of the life and work at the three sites and headquarters and
how the original, mainland radar system was commissioned, operated,
maintained and developed.</p>
      <p id="d1e112">The initial planning and development of the association before the official
inauguration in 1981 has already been described by five of the “founding
fathers” of EISCAT (Hultqvist, 2011; Oksman, 2011; Holt, 2012; Bauer et
al., 2013; Haerendel, 2016) from their respective national perspectives.
My story picks up where those contributions end. It is by and large based on
my own notes and recollections and does not claim to be comprehensive –
there are undoubtedly many aspects of life at EISCAT that have been
forgotten or passed over. To fill in some of the holes, I have relied on
already available published information. EISCAT's Annual
Report series, which provides continuing coverage of the system developments
and the scientific production from the start, and which is now available on
the EISCAT website <uri>http://www.eiscat.se</uri>, last access: 27 January 2022, has been particularly
helpful. Interested readers looking for more detail are encouraged to visit
the website and do their own research.</p>
      <p id="d1e118">The paper is subdivided into this Introduction and a further 14 sections. To
set the stage for the technical part, Sects. 2 to 7 are dedicated to the
most important component of the system, the staff, without whom nothing
would have been accomplished, and their working conditions. Section 2
describes how the sites were organised and staffed according to the initial
plans and how the organisation and staffing then gradually adapted to the
actual demands, based on experience. Sections 3 and 4 cover the work and
responsibilities at the three sites, including important tasks not commonly
known in the user community but vital to the ability to maintain operations
and observations and deserving of recognition. Section 5 addresses some of
the challenges involved in maintaining a geographically dispersed,
multi-site high-tech system in the high north in the 1980s, with long
distances, national borders, limited communications, no Internet, 1970s
computer technology and a semi-Arctic climate. Section 6 briefly describes
the new tasks connected to the development of the Svalbard radar system.
Finally, Sect. 7 covers the annual review meetings and other social events
aimed at fostering and maintaining a team spirit.</p>
      <p id="d1e121">Section 8 deals with the organisation and work of EISCAT headquarters (HQ)
with special attention to the contributions of the directors and the HQ
software group.</p>
      <p id="d1e125">Maintenance and repair tasks were largely defined by the radar hardware at
the respective sites. Sections 9 and 10 therefore give overviews of the UHF
and VHF systems. The prehistory and successes of both systems are summarised,
and their shortcomings are also discussed at some length, in particular
those of the VHF system, which are known to the user community only in very
general terms.</p>
      <p id="d1e128">A very important component in making EISCAT such a successful project was
its computer system and the associated software system, EROS. Section 11
with subsections gives a description of these, how they were set up and
operated and how experiment data were recorded and processed.</p>
      <p id="d1e131">Another, possibly even more important component was the programmable
correlator. This potentially very powerful but fault-prone and
user-unfriendly device was eventually rehabilitated and its full potential
unlocked, largely thanks to the work of a dedicated site programmer and an
equally dedicated deputy director. New coding schemes were then tested<?pagebreak page3?> and
implemented, first in Special Programmes and after some time also in Common
Programmes, delivering data with a much improved rate of statistics. Section 12
with subsections summarises these developments and presents a brief rundown
of all Common Programmes as they stood in ca. 1995.</p>
      <p id="d1e134">Precise timekeeping and frequency keeping were essential to the success of the
tristatic UHF system but were non-trivial in the early 1980s; no
satellite-borne navigation system open to the public existed yet, so it had to
be based on the use of atomic clocks at all sites and several backup
systems. The maintenance and development of the timing system are briefly
described in Sect. 13.</p>
      <p id="d1e137">While the EISCAT system was established in the very sparsely populated far
north of Fennoscandia, there was still a surrounding society with which it
has had to co-exist on mutually acceptable terms. A critical aspect of this
fact proved to be the spectrum issue, details of which are not widely known
and therefore documented in Sect. 14 as a reminder to those possibly
contemplating the establishment of other active systems.</p>
      <p id="d1e140">The paper ends with some personal reflections (Sect. 15).</p>
      <p id="d1e144">All work, results and successes documented here are products of a dedicated
collective where everyone deserves equal credit. Apart from the directors,
individual staff members are therefore not mentioned by name, except in a
couple of cases where an important breakthrough can be ascribed to a single
individual. External consultants, advisors and collaborators from the user
community have been identified by name where relevant.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Site staff complement</title>
      <p id="d1e155">The staffing and tasks of the three sites in Finland, Norway and Sweden were
defined in quite some detail already in the negotiation phase, subsequently
laid down in the famous “Yellow Book” (Hagfors et al., 1974) and
eventually formalised in an agreement. In Finland and Sweden, recruitment
and employment of the site staff were to be subcontracted to the
Sodankylä Geophysical Observatory (SGO) and the Kiruna Geophysical
Institute (KGI, later IRF) under a “matrix organisation” arrangement: site
staff would belong to the line organisations of the local host institutions
but work full time for EISCAT under direct control and supervision by
headquarters and be charged with operating and maintaining the radar
equipment at their respective sites, thus effectively forming the
operational branch of EISCAT. This scheme guaranteed the site staff the same
benefits and social security as individuals in comparable positions in each
host country, securing them credits towards their national pension plans and
also offering a degree of job safety at the end of the planned lifetime of
the association (13 years). In Norway, the setup was initially different; in
addition to being the Norwegian shareholder, the Norwegian research council,
NAVF, would also employ the Tromsø site staff. This arrangement was
gradually brought in line with that of the other two host countries, such
that by 1995 the responsibilities for the staff were finally completely
transferred to Tromsø University.</p>
      <p id="d1e158">According to the Yellow Book, the total number of staff required at
Tromsø during the first years was estimated to be 11, at Kiruna 5 and at
Sodankylä 3 – but as the system was being constructed, these estimates
were soon revised upwards. Initially, a site manager position was explicitly
foreseen only for Tromsø but was also soon introduced at the other
sites. This position was the embodiment of “middle management”. A skilled
engineer by training, with both technical and management experience, the
site manager was responsible toward HQ for all operational matters,
including maintaining the equipment, executing the operational schedule and
setting up and executing a site budget. At the same time, he was responsible
toward the host institute for all personnel matters and toward his own staff
for managing all day-to-day tasks like the scheduling of shift work and looking
after everybody's wellbeing. Previous management experience was probably
decisive in the selection of the first group of site managers, who were all
recruited from outside the host institutes.</p>
      <p id="d1e161">Located at Ramfjordmoen, about 30 km south of the city of Tromsø and the
university, the Tromsø site needed a range of skills that would enable it
to function as a self-contained research station. To that end, service and
support positions like a secretary, a caretaker and a combined
mechanic–janitor were established. A substantial engineering staff, eight to nine positions, was going to be required for operating, maintaining and repairing
the two transmitters and their accompanying antennas, receivers and signal
processing systems. There was also a site scientist, responsible for the
scheduling of the radar, the operation of the Common Programmes and the
support for visiting scientists coming to operate Special Programmes. When the
heating system (Rietveld et al., 1993) was transferred from the
Max-Planck-Institut für Aeronomie (Germany) to EISCAT in 1992, a
dedicated heating scientist position and two engineering positions (later
reduced to one for budgetary reasons) were added to the Tromsø staff
complement.</p>
      <p id="d1e164">A much smaller staff complement had been planned for the remote sites, as
these would be located relatively close to their host institutes and able to
draw on service functions from these. Once in the operations phase, two
engineers assisted by one technician would keep the sites running and
operate the Common Programme. In addition, they would handle system-wide
maintenance, repair and improvement of the electronics subsystems developed
at the respective site, viz. the receivers and timekeeping systems (Kiruna)
and the analog to digital converters and matched filters (Sodankylä).</p>
      <p id="d1e168">At Kiruna, the staff complement did indeed end up as foreseen, but the
Sodankylä one was quickly augmented by two resident site scientists.</p>
      <p id="d1e171">As the project got underway, it soon became clear that the amount of
software and computer support required at the<?pagebreak page4?> sites had been underestimated
from the beginning, and each site eventually got a site programmer. That job
title was really a bad misnomer, as the duties in practice did not only
comprise coding but also – and perhaps more importantly – the maintenance of
the site computer systems, including peripherals and operating system
software; today a more proper job title would have been “software system
engineers”.</p>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Tasks during operations</title>
      <p id="d1e182">During radar operations, work at Ramfjordmoen went on around the clock.
Operation outside regular working hours (nights and weekends) required the
engineering staff to work shifts. Since transmitter operation involved high
voltages and possibly dangerous troubleshooting, there always had to be two
persons scheduled per shift, one of whom had to be a competent transmitter
operator. In addition to keeping the transmitter running, the receiver and
data recording systems also had to be monitored and data tapes changed at
regular intervals. Visiting scientists, coming to Tromsø for experiment
campaigns, often volunteered to join the night shifts to off-load this duty
from the staff. After a few such night shifts, they could return to their
home institutions with an appreciation of the challenges involved in
operating the system and the skill and commitment of the site staff.</p>
      <p id="d1e185">Restarting the system after a massive “crowbar” (explained below) was a
dreaded task during night shifts. The transmitter always went down to
standby following a crowbar and had to be brought back up to full power
gradually. Voltage transients caused by the current pulse through the spark
gap made the lights flicker and often crashed both the correlator and the
computer systems, necessitating a restart of the running experiment. If the
crowbar had been triggered by a spontaneous klystron arc during the receive
part of a radar cycle, the receiver front-end amplifiers up in the antenna
hub room were very often damaged, forcing a total stop until repairs could be
effected during normal working hours – getting at them required a climb up
two ladders to the upper antenna platform, 20 m above ground!</p>
      <p id="d1e188">At the remote sites the operations-related workload was much less demanding.
There was no transmitter to worry about, and the amount of raw data recorded
was much less than at Tromsø, so a data tape could last for a full 24 h. During the first few years there was nevertheless a night watch kept,
as the correlators frequently stopped or crashed, requiring a manual
restart. But as the system gradually stabilised and the remote monitoring
and control features of EROS began to be trusted, more and more of the
night-time operations were monitored from Tromsø. Local staff was then
kept on call and could be alerted if needed.</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Maintenance, repair work and hazards</title>
      <p id="d1e200">The other side of the site work, one that most visitors only got
superficially exposed to, was the maintenance and repair of the transmitters
and antennas (addressed later). Transmitter work was performed under
conditions largely similar to those encountered in heavy industry – dirty,
heavy and partly dangerous. Troubleshooting and repairs often had to be
performed under time pressure.</p>
      <p id="d1e203">The transmitter hall was a large industry-type sheet metal building, housing
two big oil-filled tanks for the klystrons and other high-voltage
components. There was also a large high-voltage capacitor bank and the
famous crowbar. A travelling crane, spanning the full length of the
hall, was used to extract the klystrons from the tanks when they or some
related high-voltage component had to be serviced. This was a delicate job;
the VHF klystrons were about 5 m tall and very heavy but at the same
time fragile and very intolerant of mechanical stress. Reinserting them in
their sockets without breaking vacuum required precision and patience.</p>
      <p id="d1e206">The modulator decks with their specially processed switch tubes were also
located in the tanks, fully immersed in the oil. A weak point in the
transmitter systems, they frequently had to be hoisted, left to drip off and
repaired or replaced.</p>
      <p id="d1e209">While the klystrons and the other equipment in the oil tanks constituted
work hazards mainly because of their bulk and mass, the potentially most
dangerous, even lethal, component in the transmitter hall was the capacitor
bank (Fig. 1, left). Its purpose was to supply the current for the
klystron beam when the transmitter pulsed while at the same time
maintaining the beam voltage. It was constructed in two sections, one 80 <inline-formula><mml:math id="M1" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>F
and one 20 <inline-formula><mml:math id="M2" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>F, that could be paralleled if required and charged to over 100 kV. When fully charged, it contained about a quarter of a kilowatt-hour or
the equivalent of about 200 g of TNT. Since an uncontrolled discharge
inside the tube could dump all this energy into a plasma arc and instantly
ruin the klystron, there was a protective mechanism, the crowbar (Fig. 1, right), installed. This was a triggered spark gap, connected across the
capacity bank, that was fired if the monitoring systems detected a rapid rise in
the klystron beam current. A massive spark then formed in a couple of
microseconds, effectively short-circuiting the capacity bank and dropping the
klystron beam voltage to only a few hundred volts, thus eliminating any
possibility of a tube arc – but the spark also generated an almighty bang
that could be heard throughout the site. As a safety precaution, the
capacity bank and the crowbar were enclosed in a netting cage with interlocked
gates that would break the high voltage and trigger the crowbar if opened
while the system was operating.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e231">Left: an overview over part of the capacitor bank. Right: the
crowbar spark gap. Photo courtesy of Ralf Larsen, Tromsø, formerly
with EISCAT.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hgss.copernicus.org/articles/13/1/2022/hgss-13-1-2022-f01.jpg"/>

      </fig>

      <p id="d1e240">Another, invisible occupational hazard was X-ray radiation. When the
transmitters were operating, the klystron beam collectors emitted X-rays
with a maximum energy of 80–100 keV; most of the radiation was however the
result of multiple scattering and therefore of much lower energy. The
collectors were enclosed in lead shields, but even so,<?pagebreak page5?> some radiation leaked
out, and the engineering staff had to take care not to expose themselves
unnecessarily. Everyone working around the transmitters wore film dosimeters
that were checked at regular intervals by the radiation safety department at
Tromsø University, a task delegated there by the Norwegian Radiation
Protection Authority (Statens Strålevern).</p>
      <p id="d1e243">A frustrating aspect of the maintenance work was the fact that the original
transmitter systems, as well as the 32 m UHF antennas, were designed and
constructed according to the SAE engineering standards dominating in the United States.
Pump motors, including the big motor for the main coolant pump, were
designed for US voltages and required extra transformers to adapt them to
the Norwegian power system. Nuts and bolts throughout the transmitters had
UNC or UNF threads and were specified to the nearest <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">64</mml:mn></mml:mrow></mml:math></inline-formula> of an inch,
requiring SAE socket wrenches instead of the metric ones used on all
European-made equipment. Pipe sizes were likewise specified in inches,
keeping the site mechanic busy with devising ad hoc adapters when the main
coolant loop plumbing developed a leak – which it did from time to time with
sometimes spectacular results. But when the cast-iron casing of the original
main coolant pump developed a crack, the whole pump was replaced with a
European-made unit. From then on, as components began to fail, they were
replaced with functional equivalents conforming to European standards
wherever possible, which eventually simplified the maintenance task a lot.</p>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Travel on the job</title>
      <p id="d1e267">Maintaining the tristatic UHF facility required a lot of travel between the
sites. During the build-up phase and the first 3 years of operation, the
only road connection from Kiruna to Tromsø was via a narrow two-lane road
through Finland, from Karesuando to Kilpisjärvi (see Fig. 2), a
distance of about 410 km, for the most part speed-limited to 80 km/h and
initially involving a crossing of the Muonio River by road ferry at the
Swedish–Finnish border at Karesuando; the bridge there was only built in 1980. This was shortened to about 330 km when the new E10 road from Kiruna
to Narvik was opened in September 1984. Sodankylä to Kiruna is about 330 km, and Sodankylä to Tromsø is almost 480 km. These distances made it
impractical to visit one of the other sites for business and return the same
day. Most trips tended to become at least 2 d affairs, except during the
summer months when there was daylight around the clock – but all sites had
facilities for staying overnight. During experiment campaigns, these were also
heavily used by visiting scientists. The Kiruna site building had a guest
room that could house two, visitors to Sodankylä could use the
Geophysical Observatory guest rooms and in Tromsø a prefabricated
barracks-type building, affectionately called the “Hilton” and containing
eight guest rooms, a kitchen and a common room area, was erected within
walking distance from the site.</p>
      <p id="d1e270">In the wintertime, driving was sometimes downright hazardous, most of the
distance having to be covered in darkness and often with drifting snow
reducing the visibility to a few metres. There was also a constant risk of
encountering reindeer in the road. No staff were ever involved in serious
accidents, but breakdowns occurred now and then and could result in long
delays. My first trip to the Sodankylä site in mid-winter 1982 is a case
in point – a front wheel bearing breakdown in Pajala, about halfway, almost
ended my trip in the ditch but thankfully only resulted in an unplanned
visit to the only garage in town and a total travel time of 18 h for an
average speed of 18.3 km/h.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e275">Outline map of the EISCAT KST geographical area (from the 1984
EISCAT Annual Report). The initial road connection between the Tromsø site
and the remote sites entered Finland at Kilpisjärvi, close to
Treriksröset, the point where the Swedish, Finnish and Norwegian borders
meet. From there it continued southward on the Finnish side of the
Swedish–Finnish border. The connection to Kiruna branched off and crossed
the border at Karesuando, about 110 km from Treriksröset, and the road
to Sodankylä branched off at Muonio, 80 km farther on.</p></caption>
        <?xmltex \igopts{width=227.622047pt}?><graphic xlink:href="https://hgss.copernicus.org/articles/13/1/2022/hgss-13-1-2022-f02.png"/>

      </fig>

      <p id="d1e285">Another factor affecting travel between the sites was the customs control at
the borders. Until Finland and Sweden joined the EU on 1 January 1995, and
free mobility of goods throughout the EU was established, transport of
goods between the three host countries was strictly controlled. This put an
extra burden on the staff when preparing for a trip because all
instruments, test equipment, tools and spare parts transported between the
sites were considered merchandise and had to be declared; even the data
tapes recorded in Tromsø and Sodankylä that had to be physically
transported to Kiruna for processing at HQ were regarded as a sellable
commodity! Every border passage involved a stop for customs control, at
which the driver was expected to hand in a set of customs declarations
prepared before the trip and containing a detailed classification and
evaluation of the goods transported. During the first few years, before the
customs personnel had become comfortable with the EISCAT transports, the car
could even be subjected to an inspection. On the return trip, the exercise
had to be repeated to ensure that no goods that had been allowed into a
country free of duty were left there; everything had to be brought back out.
In addition, a language barrier existed at the Finnish border checkpoints in
Karesuvanto and Kolari. The staff there spoke very little English and if
something was unclear and there were questions asked, things could get a bit
stressful. Luckily, one of the Kiruna site engineers spoke Finnish, so when
major<?pagebreak page6?> shipments across the Finnish border had to be made, he was often doing
the driving.</p>
      <p id="d1e288">Once Sweden and Finland had joined the EU, all controls at the
Finnish–Swedish border disappeared overnight. A customs border still existed
into Norway, but handling at the Riksgränsen and Kilpisjärvi
checkpoints soon became quite streamlined.</p>
</sec>
<sec id="Ch1.S6">
  <label>6</label><title>Development work for the EISCAT Svalbard Radar (ESR) project</title>
      <p id="d1e299">Following the principle decision in 1990 by the Council, the association's
governing body, to develop a Svalbard radar, considerable time and effort
was spent on a series of feasibility studies. These eventually led to the
formal decision at the end of 1992 to begin the construction, following a
hardware-driven strategy. The plan was to do as much of the hardware
development work as possible in-house, using the staff and expertise already
available at the sites. Areas where this was possible and advantageous
included the receivers, the signal processing systems and the low-level
digital control systems. The work was divided up between the sites along the
same lines of responsibility as drawn up at the start of the mainland system
and maintained thereafter: the radar controllers were assigned to Tromsø,
the analogue part of the receivers and the transmitter exciter to Kiruna and
the receiver digital back end to Sodankylä. Programming of the digital
signal processor VME boards and overall integration into a VME environment
became the responsibility of the deputy director with lots of help from the
Sodankylä site scientist. About one and one-half position at each site,
and a sizable fraction of the deputy director's work time,
were tied up in this development work for nearly 4 years. The involvement
of Tromsø staff gradually increased, particularly related to electrical
power and transmitter installation work – the site mechanic worked on-site
at the ESR for long periods – and for some time the mainland operation had
to be restricted due to a resulting shortage of resources. But the end
result was an indisputable success – the ESR saw first light on 16 March 1996, on schedule and within budget! It has operated reliably ever since.
The technical details of the ESR project and the very first results are
published elsewhere (Wannberg et al., 1997).</p>
      <p id="d1e302">Once the ESR had stabilised, and manpower and capital investments into the
mainland systems could be contemplated again, in 2002 the old ADC/correlator
systems were scrapped and replaced with new digital back ends, patterned on
the ESR signal processing system but using embedded UNIX computers for the
correlation computations instead of DSP chips and including new ESR-type
radar controllers. The resulting performance improvement was dramatic,
allowing for the use of new and complex modulation schemes on both the VHF and
the UHF, generally improving the rate of statistics and minimising the
digital noise level and failure rate.</p>
</sec>
<sec id="Ch1.S7">
  <label>7</label><title>Annual review meetings and Christmas parties</title>
      <p id="d1e313">Many individuals working at the sites had few occasions to travel on the job
and so not much opportunity to get to know their colleagues at the other
sites and learn about their work first-hand. To help team building and
to strengthen the team spirit, a review meeting of the whole staff was
therefore held every year. This was a 3 sometimes 4 d combined
work and socialising event, at which everybody had an opportunity to present
their work in conference-format sessions and contribute to plans for the
upcoming year in working groups, but the schedule also contained plenty of
time for skiing, fun and play. The venue rotated between Finland, Norway and
Sweden in a 3-year cycle. Local arrangements were as far as possible
handled by the staff of the host country site, with help from HQ as needed.</p>
      <p id="d1e316">During the first decade, the meeting was always arranged during the best
skiing season in mid-March, when the sun had returned and the snow still lay
metre-deep, at a resort not too far away from the local site and if possible
with alpine slopes nearby, for example, Levi in Finland and Riksgränsen in
Sweden. In later years, the meeting was often held in early autumn. In 2000,
the meeting was held on board a<?pagebreak page7?> Hurtigruten ship during its regular
scheduled trip from Tromsø to Vardø and back, with an excursion to the
North Cape included as part of the social programme.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e321">Group photo of the EISCAT staff at the 1985 annual review meeting
in Abisko, Sweden. Most of those pictured here have long since left the
association and/or are now retired, but one individual is still working for
EISCAT! From the 1985 EISCAT Annual Report.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hgss.copernicus.org/articles/13/1/2022/hgss-13-1-2022-f03.jpg"/>

      </fig>

      <p id="d1e331">On the last night there was always a banquet with lots of good food, a few
speeches and a small ceremony where new team members were welcomed into the
EISCAT family and old staff members acknowledged through the awarding of
pins for 2, 5 or 10 years of service.</p>
      <p id="d1e334">Proceedings were compiled after each review meeting and distributed
internally. They frequently contained highly detailed technical material,
served as very useful handbooks and reference material for the staff and
were often referenced in the annual reports. They could be of great
historical interest but unfortunately do not seem to have been saved in
digitised form, at least not yet.</p>
      <p id="d1e337">The annual Christmas parties were highly appreciated social events. They
were arranged locally at the three workplaces, in Kiruna jointly between HQ
and the site, a couple of weeks before the holidays, and took the form of a
lunch or a dinner with lots of traditional Christmas food in a cosy local
restaurant, followed by relaxed socialising by the fireside. Spouses were
also invited.</p>
</sec>
<sec id="Ch1.S8">
  <label>8</label><title>Headquarters</title>
      <p id="d1e348">For legal purposes, the EISCAT Association was established as a Swedish
not-for-profit foundation (stiftelse) with its seat in Kiruna. Its executive
branch, headquarters, also came to reside there.</p>
      <p id="d1e351">A skeleton headquarters (HQ) was formed in 1976, establishing itself in
office space rented from the Swedish Institute of Space Physics, IRF. HQ was
in many ways organised along the same lines as the executive body of a
typical mid-size company. The director, the top official, was the “EISCAT
CEO”. He was appointed by the association's governing body, the Council,
and responsible for implementing the scientific programme as defined by
the Council and committees. He was also charged with maintaining relations with
the local bodies in Norway, Sweden and Finland hosting the EISCAT sites. His
staff included an assistant director science (ADS), responsible for the
scientific operations, particularly the Common Programmes, and reporting to
the Scientific Advisory Committee (SAC), an assistant director technique
(ADT), responsible for the technical infrastructure, a business manager,
handling the association's financial and business operations
and communicating with the Administrative and Finance Committee (AFC), and a
secretary. One or two administrative assistants (the number varied over
time) were also employed. A very important part of HQ was the
computer/software section. It was led by a head programmer, responsible for
directing and overseeing the development and implementation of the software
required to control the radar system, run experiments and record the data.
The software section also handled the archiving of data, production of data
copies and distribution of these to the users.</p>
      <p id="d1e354">For the first years, work at HQ focussed on the actual establishment and
construction of the radar system. The development, installation and
commissioning of the antennas and transmitters were contracted out to
industry. Monitoring and guiding the orderly progress of these contracts
took up much of the director's time. Since most of the heavy equipment was
being installed at the Tromsø site, the ADT was permanently stationed
there until the end of the build-up phase.</p>
      <p id="d1e357">At the same time, development of the application-specific software required
to control the radar and the implementation of the Common Programmes was
addressed by the association's own staff – a logical move,
since the EISCAT system was the first of its kind, and no comparable
installation using Norsk Data computers existed (see Sect. 10). In this
work, the head programmer and his group were supported by the site
programmers, each taking charge of a subset of the system and application
software. The task of designing and realising the initial Common Programmes
largely fell to the ADS, supported by expert users from the member
countries, notably France and the United Kingdom.</p>
      <p id="d1e361">In an attempt to keep own staff and eagerly waiting ionospheric scientists
in the member countries up to date on the progress, a very ambitious EISCAT
Newsletter was launched under the editorship of the ADS. Unfortunately, it
seems that the workload at HQ soon overwhelmed the staff, and the newsletter
just stopped. Very few copies are known to remain. I have a copy of no. 3,
which is full of great information about the radar system and complementary
instruments, like the STARE radar and the GEOS II and ISIS-2 satellites. It
was probably the last issue.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e366">Front page of the EISCAT newsletter, no. 3, issued by HQ in April 1978. Scan of my personal copy.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hgss.copernicus.org/articles/13/1/2022/hgss-13-1-2022-f04.png"/>

      </fig>

      <p id="d1e375">I had the opportunity to work under the association's first four directors,
whose terms span the scope of the present paper. Looking back, it is clear
that each of them was uniquely<?pagebreak page8?> equipped to handle the tasks that dominated
their respective time in office. As the first director, Tor Hagfors led the
build-up phase. It would have been impossible to find a better qualified
candidate. Hagfors was a brilliant theoretician and one of a small group of
people who had derived the theory of incoherent scatter independently of
each other. He also had extensive experience in science administration;
before starting with EISCAT in 1975, he had served as the director of the
Jicamarca and Arecibo radar observatories.</p>
      <p id="d1e378">In 1982 Hagfors left for new challenges in the United States and was succeeded by
Murray Baron, a radar scientist from SRI International in Menlo Park,
California. Baron had a long career in ionospheric radar and had been deeply
involved in the design, implementation and exploitation of the Chatanika,
Alaska, ISR system. At this point in time, HQ was working on solving the VHF
transmitter issue; Aydin, the California-based company contracted to build
the transmitter, was in difficulties and lagging seriously behind the
delivery schedule (see Sect. 9). Coming from a workplace located in the same
high-tech area and with an intimate knowledge of US law and business
practice, Baron was the ideal person to resolve the issue. Under his
guidance, the VHF transmitter was finally delivered in 1984, and all remaining
business dealings with Aydin terminated.</p>
      <p id="d1e381">In 1985 the director's chair was filled by Jürgen Röttger of
MPI Lindau. Röttger had a solid background in middle atmosphere physics
and MST (mesosphere–stratosphere–troposphere) radar. He was no newcomer to EISCAT – he had already served as ADS
under Baron between 1982 and 1984 and then left for a short stay at
Arecibo, from where he was recalled. He took over an EISCAT that had started
to function reasonably well and led it through an extremely productive
period, including the design and construction phase of the Svalbard radar
(ESR) project and culminating in the commissioning and inauguration of the
ESR in 1996. He was an extremely committed leader, who took a deep personal
interest in almost all aspects of the association's work and eventually came
to be the longest serving Director, leaving in 1997 after 11 years in
position. His personal scientific interests manifested themselves in an
increased emphasis on the development and operation of experiments optimised
for mesosphere observations, with the long series of observations of polar
mesospheric summer echoes (PMSEs) perhaps the most important contribution.</p>
      <p id="d1e385">History then repeated itself – Röttger was succeeded as director by
Tauno Turunen, who had been ADS from 1984 to 1987 and devised, programmed
and tested the series of GEN programmes that came to be templates for nearly
all EISCAT experiments for more than 10 years. Turunen's professional
affiliation was with the Sodankylä Geophysical Observatory. He was
primarily a hardware man with a background in ionosonde technology and radar
coding and had been involved with the initial setting up of the
Sodankylä UHF site. He had also served on different committees in an
expert capacity. During his time as director, he oversaw the completion of
the ESR 42 m antenna project and supervised a major rehabilitation of the
mainland systems, which out of necessity had not been fully maintained
during the ESR build-up phase. He also continued his experiment design work,
making full use of the new signal processing capabilities introduced as part
of this process.</p>
      <p id="d1e388">When the IRF in 1999 began a major rebuilding project, the wing containing
the HQ offices was targeted for demolition. After a crash investigation of
different alternatives, the whole HQ operation moved into rented office
spaces in the town centre of Kiruna, where it remained until 2007. Turunen
thus came to spend most of his term in these new surroundings. He left
EISCAT in 2002 and was succeeded by Tony van Eyken, who had been selected to
lead the association into what could perhaps be termed the “Svalbard radar
harvest season”. But that is a different story, which is not addressed here.</p>
</sec>
<?pagebreak page9?><sec id="Ch1.S9">
  <label>9</label><title>The UHF system</title>
      <p id="d1e399">Looking back through the earliest documentation, it is obvious that the
steering group was convinced of the feasibility of the UHF system very early
on through contacts to industry and already operating ISR systems. The
Yellow Book contains a highly technical description of the proposed
transmitter, based on a feasibility study for the St. Santin radar and
complemented by a detailed costing; the actual transmitter was largely
patterned on this proposal. A detailed description of the antenna and
receiver system planned at the time is also presented there, but this was of
course superseded by the later decision to go for fully steerable antennas
at all sites.</p>
      <p id="d1e402">The UHF transmitter actually did perform largely as planned already from the
start and soon evolved to a point where the hardware was regarded as
predictable and reliable. It was planned as a two klystron system, but
initially only one tube was installed. It was then run with just one
klystron until the output power of the second of the two original VA862
Varian klystrons started to drop.</p>
      <p id="d1e405">The VA862 design was special in that it allowed for the transmission of very
long pulses of up to 10 ms duration. This was the result of deliberations in
the planning stage, when it was believed that quasi-continuous-wave (CW) illumination of the
beam intersection volume would be required to get acceptable velocity
statistics at the remote stations. But by 1982, data from CP-0-type
experiments clearly demonstrated that good velocity estimates could be had
using a common <inline-formula><mml:math id="M4" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 350 <inline-formula><mml:math id="M5" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>s pulse for all sites, so the long-pulse
capability was never put to serious use, and when performance requirements
for new klystrons were drafted, the maximum pulse length was set at 2 ms. A
proposal by the Thomson corporation for a klystron with better efficiency
than the old Varian tubes was accepted, and an order for two tubes was
placed. Since the transmitter oil tank and much of the waveguide were already
prepared to accept two tubes, both new klystrons were installed upon
delivery and have since been run in parallel for a typical output power in
the order of 2 MW; 3 MW was theoretically possible but rarely achieved
because of high reflected power limitations.</p>
      <p id="d1e423">It was well understood that the UHF signals backscattered from the
ionosphere would be very weak much of the time. The cosmic noise background
would not be a problem – at 933 MHz the sky noise temperature is typically
10–15 K – but in the receiver, the signals would have to compete with
noise generated in the first amplifier stage, typically 10 to 100 times stronger than the signal, resulting in signal-to-noise ratios of only a few
percent. A prime design target for the UHF receiver was therefore the lowest
possible noise temperature. It was clear that to reach the remote station
target system noise temperature of <inline-formula><mml:math id="M6" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 30 K, a cooled receiver front
end would be mandatory. On advice from the radio astronomy community, the
designers chose a solution based on a wideband, high gain, cryogenically
cooled parametric amplifier, designed and built by AIL of Long Island, United States.
This device could deliver about 60 dB of gain over a 30 MHz wide band while
adding less than 20 K to the overall system noise. Unfortunately, it also
turned out to be extremely sensitive to overload and ill-suited for use in a
radar system. At Ramfjordmoen, klystron arcs resulted in several burnt-out
amplifier upconverters. These could not be repaired locally but had to be
shipped back to AIL, causing major disruptions of the schedule. To maintain
operation, the Tromsø system had to rely on uncooled transistor
amplifiers with much poorer noise performance. These were eventually
replaced by GaAsFET amplifiers designed and built at the Kiruna site, which
brought the system noise down to 90–100 K. At the remote sites, the paramps
were kept in operation for several years, but when the first mobile phone base
stations started up in Kiruna and Sodankylä, their wide passband proved
to be a liability; they went into saturation and had to be replaced by an
in-house designed cooled GaAsFET amplifier system. The cryosystems were
maintenance intensive and occupied a lot of the responsible engineer's
work time.</p>
      <p id="d1e434">Another shortcoming of the initial receiver design manifested itself very
quickly after the start of regular operations. The original post-detection
filters, located immediately ahead of the ADC, had been designed with
insufficient regard to the need for phase linearity and were also plagued
with DC offset problems. Following a critical report from a study group led
by Turunen (Turunen et al., 1981), new filters were designed based on
experience from the Sodankylä ionosonde and featuring optimised impulse
response for all commonly used pulse lengths. Such filters were then
produced at the Sodankylä site in sufficient numbers to allow for a system-wide
refit of all receivers.</p>
      <p id="d1e437">The 32 m UHF antennas (Fig. 3) were “wheel-on-track” Cassegrain designs,
based on a standard Intelsat-1A ground segment antenna design that had
already been built in substantial numbers but with modified feed systems to
adapt them to work at 933 MHz. The alidade (i.e. the moving structure
carrying the reflector) stood on four wheels that rode on a circular track
on top of the antenna foundation. Two of the wheels were fitted with DC
motors that drove the antenna in the azimuth plane. A further two motors,
located on a platform level with the elevation axis, drove the reflector in
the elevation plane via a massive tooth rack.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e442">The Kiruna EISCAT UHF antenna. The Tromsø and Sodankylä
antennas were identical, apart from the feed system of the Tromsø one,
that included a waveguide run with rotary joints connecting to the
transmitter. Photo courtesy of Lars-Göran Vanhainen, Swedish Institute
of Space Physics (IRF).</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hgss.copernicus.org/articles/13/1/2022/hgss-13-1-2022-f05.jpg"/>

      </fig>

      <p id="d1e451">In the Intelsat application for which the antennas were originally designed,
fast movement was not needed, as the antennas were used as the ground
endpoints of links to geostationary communications satellites and therefore
only needed to move slowly to optimise the pointing to the satellite or to
move to a stow position. The EISCAT application was quite different; an
ability to move rapidly was essential for many observations, and so the drive
motors and gearboxes fitted to the EISCAT antennas were much more powerful
than those of the ancestor antennas. It soon became obvious that this mode
of operation also resulted in a much increased need for regular service of
the drives and the antenna structures.</p>
      <?pagebreak page10?><p id="d1e454">Lubrication and routine maintenance of the drive systems was carried out by
the local site staff. They also looked after the “pintle bearing” that
kept the antenna centred on the rails. A number of plastic-coated segments,
mounted on a <inline-formula><mml:math id="M7" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 2 m diameter concrete cylinder centred on the
azimuth axis, made up the fixed part of this bearing; the moving part
consisted of four pads bolted to the alidade. The fixed pads wore out quite
fast and had to be replaced about once a year on average, but soon an
efficient routine evolved; worn-out pads were sent to Finland and
reconditioned there by a company specialising in industrial plastics.</p>
      <p id="d1e465">Major maintenance work required calling in outside help. The alidade and the
reflector backing were bolted together, and the bolts required regular
re-tensioning at a few years' intervals, a job requiring a crew certified
for climbing and high-altitude work – the top of the reflector backing was
35 m above ground! This job was therefore always contracted out. It was
normally scheduled for a period of low demand in the summer and combined
with a general overhaul of the reflector. To minimise the impact on the
regular operation, all three UHF antennas were serviced one after the other
in this manner during a single summer season whenever possible.</p>
      <p id="d1e468">Bolt tensioning could be planned for in advance, but the same was not always
true of the rail maintenance. After about a decade of operation, it was
discovered at all three sites that the concrete carrying the rails had
started to fracture in places, and the rails were settling and even coming
loose. This was a serious condition that had to be addressed promptly
whenever detected, irrespective of season or weather: the antenna had to be
locked in azimuth, the fracturing concrete chiselled away from underneath the
rail and new frost-proof, rapid-curing concrete poured in, while monitoring
that the section under repair ended up level with the rest of the rail. This
work was always performed by contractors but closely monitored by the site
staff to ensure correct rail alignment.</p>
      <p id="d1e471">For some time, the safety of the Finnish UHF antenna, located at the
Tähtelä observatory about 10 km south of the town of Sodankylä, was in
question due to actions by entities outside EISCAT control. This antenna
stands on sandy soil just 80 m from the east bank of the Kitinen River. When
the association was established, the river and its tributaries were still
unregulated, but in 1988, Kemijoki OY, the company possessing the water
rights, applied for a permit to construct a hydropower plant at Kurkiaska,
about 3 km downstream from the observatory. This involved damming the river
and raising the water level by about 6 m, so creating a water
reservoir stretching tens of kilometres upstream from the dam. As soon as
EISCAT got to know about the project, a strong statement of dissent was
submitted to the water rights court; if the river were allowed to rise to
the level requested in the project plan, the ground water table at the
antenna would rise to almost 2 m above the foundation footplate! This
would introduce a risk for frost heave and in the worst case endanger the
long-term stability and operability of the antenna.</p>
      <p id="d1e474">Geotechnical experts were called in to consult both parties and long
negotiations ensued. In the end Kemijoki OY agreed to a damming limit nearly 3 m
lower than first planned for, which ensured that the ground
water table at the antenna would always be at least a metre below the bottom
of the foundation. The company also agreed to put in insulation and a
heating cable all around the foundation to protect against frost heave and
to cover the operating costs of the heater for the lifetime of EISCAT. This
agreement was made legally binding on Kemijoki OY by a decision in the water
rights court on 29 December 1988. The heater and the insulation were put in
the next summer. No problems related to the damming have been noticed since.</p>
</sec>
<sec id="Ch1.S10">
  <label>10</label><title>The VHF system</title>
      <p id="d1e485">The 1971 feasibility study (the Green Book) put forth strong arguments
for a VHF system. Foremost among these was the ability to make measurements
in conditions of very low electron density, in the mesosphere and the bottom
of the E layer and in the topside ionosphere at altitudes well above 1000 km, where it was expected that it would detect the theoretically predicted
“polar wind”. The Green Book only contained a rough outline of the
envisaged system, but the concept soon matured into a very ambitious design,
comprising a 5 MW dual klystron transmitter, a <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:mn mathvariant="normal">120</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> m parabolic trough
antenna (Fig. 4), steerable in the meridian plane between 30<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N–60<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, and a high-power RF switchyard, enabling operation in two
distinct modes (Mode 1 and Mode 2). An overview of the system as first
implemented is given in Baron (1986), but a recapitulation of its most
important features is included below as a background to the long, costly and
frustrating series of mishaps described in the following.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e520">The EISCAT VHF parabolic cylinder antenna at Tromsø. It is
constructed as four individually tiltable <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:mn mathvariant="normal">30</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> m reflector–feedline
segments, which however must be electrically operated either as a single
<inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mn mathvariant="normal">120</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> m aperture (Mode 1) or as two independent <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mn mathvariant="normal">60</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> m apertures
(Mode 2). Photo courtesy of Lars-Göran Vanhainen, Swedish Institute of
Space Physics (IRF).</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hgss.copernicus.org/articles/13/1/2022/hgss-13-1-2022-f06.jpg"/>

      </fig>

      <?pagebreak page11?><p id="d1e565"><?xmltex \hack{\newpage}?>Mode 1 was optimised for maximum sensitivity. One klystron would drive all
128 horizontal dipoles in the antenna feed, and the other klystron would
drive all 128 vertical dipoles, making it possible to transmit either
linearly or circularly polarised signals and to change the polarisation on a
pulse-by-pulse basis. With separate receiver chains for the two sets of
dipoles, both total signal power and spectrum and Faraday rotation phase as
functions of range could be recovered. In Mode 2, the antenna would be
electrically split into two <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mn mathvariant="normal">60</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> m “half antennas”, configured for
circular polarisation and fed by one klystron each. The two antenna halves
could then be independently pointed in different directions both in
elevation and in azimuth, effectively creating a dual beam system at the
expense of sensitivity. However, for either mode to work as intended, there
had to be two working klystrons in the transmitter, and precisely this
turned out to be easier said than done.</p>
      <p id="d1e582">On 2 March 1976, EISCAT placed a contract for its transmitters with the
California-based Aydin Corporation. This was to be a turnkey deal, with
Aydin handing over a fully working transmitter system by November 1978. At
the time, no high-power klystron manufacturer could demonstrate a tube
meeting the EISCAT requirements, but Varian associates of Palo Alto offered
to develop a 224 MHz, 3 MW tube by extrapolating from a design for a
slightly different frequency. This was accepted, an order for three
klystrons was placed and after construction and ageing at Varian these were
delivered directly to Aydin for integration in the partially completed VHF
transmitter.</p>
      <p id="d1e585">But from then on, things did not progress smoothly. At the end of 1982, Aydin
had fallen behind the project plan by almost 3 years, two of the Varian
klystrons had failed during testing and the third was performing well below
agreed specifications. The transmitter was finally delivered to Tromsø in
1984, and following this the contract with Aydin was terminated.</p>
      <p id="d1e588">In parallel, EISCAT had started searching for an alternative klystron
supplier. In 1983, the Valvo division of Philips was contracted to supply
two klystrons with better specifications than the original Varian tubes.
Delivery of the first Valvo tube, YK1320/1, was planned for December 1984
but slipped into early 1986, which allowed it to be immediately installed in
the VHF transmitter; this had by then been operated at up to 2.5 MW with the
only remaining Varian klystron.</p>
      <p id="d1e591">The Valvo tube worked but did not meet the performance requirements. It
could be operated at 90 kV beam voltage, delivering about half of the
contracted output power, 1.2 MW, but on raising the beam voltage further, it
started arcing; not even a 300 h ageing process improved this behaviour.
Tore Wessel-Berg of NTH and Jim Tallmadge of SRI International,
both high-power klystron experts, were called in to evaluate the situation
in collaboration with the Valvo engineering team. After a thorough analysis,
it was concluded that the tube design was basically sound, but a number of
modifications were required to make it operate stably at full power, all of
which would require the tube to be returned to Valvo for rebuilding. The
proposed modifications could be directly incorporated into the second
klystron, still under production at the Valvo plant. Left with no
alternative, the Council resolved to let Valvo modify the klystron according to
the expert group recommendations.</p>
      <p id="d1e594">Meanwhile, at the end of 1986, the Tromsø site staff succeeded in running
the system with both klystrons (the Valvo and the Varian), albeit at very
low power. The full antenna was now used in experiments for the first time,
and very strong, spectrally narrow returns (later termed PMSEs) were received
from the mesosphere, which was quite unexpected. Extremely interesting
diagnostic data from a heating campaign were also recorded. These results
demonstrated that the system was indeed capable of meeting several of its
intended scientific targets.</p>
      <p id="d1e597">When I started as ADT in July 1987, my first task was to take charge of the
VHF commissioning. Progress was continually held up by problems: the Valvo
klystron developed a vacuum leak, water leaks flooded part of the
transmitter, ruining several focussing solenoids, and the last remaining
Varian klystron failed irreparably. But the second, modified Valvo tube,
which arrived in August, showed promise; it could be operated at up to 2.5 MW at better than 45 % efficiency, a major improvement on the Varian tube.
On the other hand, the contractual demand that the Valvo tubes had to be
mechanically compatible with the Varian ones had forced Valvo to make the
beam collector quite small, so it could not dissipate the full <inline-formula><mml:math id="M15" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 600 kW beam power with no RF drive present, which the Varian tube could do.
To prevent a catastrophic collector meltdown, several levels of protection
had to be introduced before Valvo would release the<?pagebreak page12?> tube for experiment
operation. To that end, software safeguards were incorporated into the
TARLAN compiler, and a microprocessor-based collector dissipation monitoring
system was constructed by Tromsø site staff.</p>
      <p id="d1e608">Confidence in the klystron-based system was now rapidly evaporating, so in
1989, HQ initiated a feasibility study to consider the replacement of the
transmitter by a power-grid-tube-based system. Companies active in the
broadcast and particle accelerator segments were approached, on-site
meetings with technical representatives were held and HQ staff visited
several accelerator facilities using megawatt-class gridded tubes.
Impressions were positive, and the concept was seriously considered for a
while. However, when the first Valvo tube was returned to Tromsø in 1990
after rebuilding, limited dual klystron operation became possible again, and
the transmitter replacement programme was put on indefinite hold. But before
long, new klystron problems arose that led to a second rebuild of tube
YK1320/2, a number of costly consultancy visits from SRI and the full-time
involvement of two–three site staff for nearly a year. It was only in late
1991, 10 years after the inauguration, that the VHF transmitter started to
behave somewhat reliably, and to achieve this, the Faraday rotation
capability first had to be given up due to frequent malfunctioning of the
duplexers and receiver protectors.</p>
      <p id="d1e611">With two functioning klystrons, the system could now be run in both modes.
Mode 2 was put to good use in experiments designed for measuring the
ionospheric convection velocity field over a wide area to the north of
Tromsø. With the VHF antenna pointed to its lowest elevation, 30<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, and phased to generate two beams, one due north and the other
approximately normal to the L shells, Doppler velocities could be derived
for a series of range gates along both beams and combined to generate two
components of the 3D velocity. The third (semi-vertical) component could be
provided by the UHF for the close-in ranges, out to some 300 km north of Tromsø, but farther towards the north,
it had to be extrapolated or was assumed close to zero. Variants of this
experiment were used as core parts of Common Programme 4. When the Svalbard radar came on the air in 1996, it was often run together with CP 4 experiments, pointing
southward into a region where the fields of view of the two systems
overlapped; under favourable conditions, the full 3D velocity field could be
determined over a large area in this way. Mode 1 suffered from a serious
operational restriction: with the antenna pointing in the field-aligned
direction and the transmitter operating at full power, radiation spillover
from the upper edge of the antenna reflector was so strong that the
Norwegian limits for public exposure to non-ionising radiation (which had
been lowered since the antenna was designed) were exceeded even a kilometre
to the south of the site. Four private homes along the main road suffered
from bad interference to telephones, TV sets and audio equipment, and
Tromsø site staff had to spend lots of time and effort on installing
shielding, filtering and better TV antennas. A number of mitigation schemes
were investigated, for example, extending the main reflector, tilting the feeder
bridge or erecting a 50 m high fence immediately south of the antenna, but
all proved too complicated and costly. In the end, full-power operation with
the beam directed to the south of vertical had to be given up. This
effectively eliminated one of the hoped-for core capabilities of the VHF
system, regular high-altitude field-aligned observations vital to the hunt
for the polar wind. Single-beam high-altitude VHF operation thus became
limited to vertical and has remained so until today.</p>
      <p id="d1e623">In the late 1980s, scientists at the Russian Polar Geophysical Institute
(PGI) obtained funding for a receiving site for the EISCAT VHF transmissions
to be built at Verkhnetolomsky on the Kola Peninsula, about 510 km ESE from
the Tromsø site. A large phased array, comprising eight <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mn mathvariant="normal">50</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> m
64-element modules and a matching dual polarisation receiver, handling both
Mode 1 and Mode 2 transmissions, was to be constructed. The system was
partially completed by 1991, and preliminary results were presented at the
fifth EISCAT workshop (Khudukon et al., 1990).</p>
      <p id="d1e638">The PGI initiative was seen as a potentially valuable complement to the VHF
system, so a number of tests were carried out, with the VHF transmitting
long pulses vertically and the PGI system receiving. However, no signals
were unambiguously identified. Time synchronisation remained a possible
uncertainty, so a so-called TV sync receiver was prepared by the Kiruna
staff and shipped to the PGI group. Unfortunately, this did not solve the
problem. After a couple of years the PGI group dispersed, and their fine
system was left unfinished. Multistatic VHF observations thus had to wait
until 2012, when the Kiruna and Sodankylä dishes were converted to VHF,
after the introduction of UMTS mobile phone systems had made continued UHF
operations impossible. At about the same time, the Finnish KAIRA
phased-array receiver system at Kilpisjärvi (McKay-Bukowski et al., 2015) also
successfully started to receive the VHF transmissions, providing an
additional baseline and multi-beam capabilities.</p>
</sec>
<sec id="Ch1.S11">
  <label>11</label><title>Computers, computing and data handling</title>
<sec id="Ch1.S11.SS1">
  <label>11.1</label><title>The Norsk Data computers</title>
      <p id="d1e657">In the early 1970s, a European big science project many times larger and
more complex than EISCAT was already nearing completion. In 1971, the CERN
Super Proton Synchrotron (SPS) project had finally got underway after years
of financial negotiations, with the goal of constructing a 300 GeV
accelerator at a total cost of up to 1150 million y1971 Swiss francs, more
than 30 times the projected y1974 cost of the EISCAT UHF system. To the
dismay in some quarters and considerable scepticism among competing computer
manufacturers, the Norsk Data Nord-10 minicomputer had been selected as the
main control computer for the new accelerator, based on the proven
reliability of its predecessor, the Nord-1, and its real-time-geared
architecture.<?pagebreak page13?> At the request of CERN, Norsk Data had provided the Nord-10
machines with a special input–output channel dedicated to communicating with
CAMAC, the de facto standard for fast nuclear and particle physics
electronics widely used at CERN. By 1976, a total of 25 Nord-10s were
already in operation at different points around the newly commissioned
accelerator ring.</p>
      <p id="d1e660">All this was noted with interest by the EISCAT planners. Many of the
processing demands of the radar system, including the need for fast and
predictable interrupt response, were similar to those of the CERN SPS, and
the possibility to use CAMAC modules to connect all project-specific
hardware to the computers was regarded as extremely valuable. Also, the fact
that CERN had already committed to the Nord-10 and would have to maintain
its machine complement for the foreseeable future guaranteed that support
for the Nord-10 would remain available during the planned time span of the
EISCAT project. Discussions with Norsk Data AS were therefore started,
leading to an order for five Nord-10 systems, two for Tromsø, one each
for Kiruna and Sodankylä and the fifth to be part financed by the IRF.
This machine was to be located in the IRF computer centre, shared between HQ
and the IRF EISCAT group and used both for software development and for data
tape copying.</p>
      <p id="d1e663">As delivered, the Nord-10 machines were equipped with 128 kB of RAM. This
was enough to get started but soon proved too little and was expanded to
256 kB. CDC Hawk cartridge disk drives, each drive the size of a small
refrigerator, provided random access storage; removable and interchangeable
disk cartridges stored 5 MB each. Data recording was on reel-to-reel <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> in., 9-track magnetic tape at 1600 Bd in.<inline-formula><mml:math id="M19" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The Tromsø site
computer had two tape stations, one each for Kiruna and Sodankylä. The
largest tape reels that could be fitted were 10.5 in. (27 cm) diameter
and contained about 2400 ft (731 m) of tape, corresponding to <inline-formula><mml:math id="M20" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 46 MB of data. To put this in perspective, a USB memory stick can offer
upwards of half a gigabyte of random-accessible storage in a <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> cm
package. There was also one graphics display at each site, a Tektronix
monochrome unit displaying the autocorrelations computed from the raw data,
using the program RTGRAPH.</p>
      <p id="d1e713">Anyone born in the 1990s or later will probably regard it as almost
unbelievable that anything useful could be accomplished in this extremely
restricted computing environment – but the Nord-10s successfully ran the UHF
system for the first 5 years! However, already early on, it became obvious
that they were not fully up to the demands raised by the quickly expanding
operations. As a temporary help, in 1984, the RAM was expanded to 512 kB,
using EISCAT-designed memory banks. Concurrently with this, Norsk Data were
introducing more powerful processing units, and in 1986, all Nord-10s were
replaced by ND-530/CX systems with 2.5 MB of RAM memory and vastly increased
hard disk capacity.</p>
</sec>
<sec id="Ch1.S11.SS2">
  <label>11.2</label><title>EROS and TARLAN</title>
      <p id="d1e724">The last Nord-10 machine was delivered in late 1977, and at that point
software development started in earnest. The plan was to make the complex
radar system user-friendly and easy to use. Under the direction of the HQ
head programmer, the software staff at HQ and the sites now set out to
develop an integrated software environment, following a basic concept
developed already before the first computers were delivered. This came to be
known as EROS, the EISCAT Real-time Operating System. A crucial step was the
construction of the command language, ELAN, whose structure and syntax were
patterned on SINTRAN, the Nord-10 operating system. Most of the EROS
software was written in Norsk Data's own Fortran dialect, ND-Fortran.</p>
      <p id="d1e727">Operator interaction with the EROS system was through ELAN commands, issued
through a simple line-oriented user interface running on an alphanumeric
terminal. This provided access to all major hardware, mechanisms to call up
and run predefined experiments from file and the ability to interact
asynchronously with a running experiment – possible because ELAN was an
interpreted language. Below the user interface level, a large number of
device-specific and mutually interacting programs and device drivers handled
individual subsystems through CAMAC. EROS was quasi-real-time-capable; the
execution of commands could be scheduled to occur at specified points in
time to a resolution of 1 s, and there was a catch-up facility that
enabled crashed and restarted experiments to seamlessly get back in sync
with the other sites. Inter-site communication was arranged via leased
telephone lines and made an integral part of EROS; it was possible to access
the systems at the other sites, send messages, check hardware and data
taking status and even command the antennas and start and stop experiments.
As the system stabilised, this functionality was gradually used to eliminate
the need for all-night staffing of the remote sites during experiments;
visiting scientists often came singly to Tromsø and ran their special
experiment campaigns from there, relying on the remote command facility to
handle the remotes and trusting them to behave – which they did most of the
time.</p>
      <p id="d1e730">While the design, development and evolution of the core EROS system and the
data handling routines resided with the HQ software group, the development
of driver software for most subsystems was assigned to the site programmers.
The UHF antenna control routines, as well as an advanced system for antenna
pointing calibration based on radio stars, were developed in Sodankylä.
Kiruna developed drivers for the receivers and real-time clocks, and
Tromsø managed the initial stages of radar controller and correlator
software development in collaboration with individuals from the
Nordlysobservatoriet and NTH Trondheim, notably Hans-Jørgen Alker.</p>
      <p id="d1e733">The original EROS system was in more or less continual evolution for about
20 years, particularly with respect to the data collection and recording
parts that had to keep up with<?pagebreak page14?> the gradually increasing data volumes and the
introduction of new storage media (fixed hard disks, Exabyte tape, etc.),
taking up a considerable fraction of all programmers' time for years into
the operations phase. Unfortunately, very little documentation of all this
development work exists in accessible form today. Two important technical
reports documenting the interfaces between EROS and EISCAT users have
survived, one teaching the user how to programme the radar using ELAN
(Armstrong, 1980) and another describing how to access the data (Farmer,
1980). This latter report shows that much thought went into defining
recording formats simplifying end user access to the data, while at the same
time adhering to established standards (ANSI X3.27 and British BS4732). As
far as the inner workings of EROS were concerned, it appears that the
programming staff relied on the Fortran source code being self-documenting,
and therefore no reports seem to have been produced; none were found in the
2020 EISCAT HQ major search and review of old documentation.</p>
      <p id="d1e737">While EROS and its component parts thus controlled most of the radar system,
two critical subsystems were handled individually: the radar controller (RC)
and the correlator. The RC generated the signals controlling the
transmitter, ADCs and Correlator during a radar cycle; the Correlator was an
application-specific, pipelined device that processed the received data on
the fly. Both were operating at microsecond or sub-microsecond time
resolution, had to be programmed at the bit level and were best left alone
once started and running. For these reasons, two unique languages, TARLAN
and CORLAN, were constructed. Both were compiled – the logical design choice
for languages constructed to control units with the ability to cause
unpredictable and even dangerous system behaviour if handled randomly.</p>
      <p id="d1e740">TARLAN was the Transmit And Receive LANguage for the RC. It had a simple
syntax – individual hardware devices were addressed by symbolic names, and
the time when an operation was to be performed was given as the number of
microseconds after the start of a cycle. All commands had to be in time
sequence, and transmitter commands had to be issued in a specific order and
with certain minimum time separation to ensure a stable output waveform.
Formally correct TARLAN code was translated by the compiler into a bit-level
file, which could be loaded into the RC. Whether the code made the radar do
what the experimenter was hoping for then had to be checked in a test run.</p>
      <p id="d1e743">The history and specifics of CORLAN are tightly interrelated with the
Correlator hardware design and therefore treated in the Signal processing
section.</p>
</sec>
<sec id="Ch1.S11.SS3">
  <label>11.3</label><title>Data handling</title>
      <p id="d1e754">The end product of all EISCAT operations was the “raw data”, the time-averaged
autocorrelation data output by the correlator, complemented by metadata
describing the system status (transmitter power, frequency, antenna
pointings, etc.). For the first few years, the extremely limited hard disk
space forced a solution where raw data dumps were continually written to
tape during experiments. Most experiments dumped data every 10 s. In
Tromsø, a large tape then lasted at least 15–16 h if the experiment
did not crash (a crash often led to a forced tape change and a restart), but
experiments running over several days involved a number of tape changes,
often during the night shifts. The data volume at the remotes was much
smaller, as only some three signal-carrying range gates, centred on the
beam intersection point, were computed.</p>
      <p id="d1e757">Initially, it had been estimated that the Tromsø system would generate in
the order of 100 data tapes per year, but as experiment operations picked up
and new coding schemes were introduced, the number of tapes grew
dramatically. As a result, tape handling expanded into an almost full-time
job. EISCAT was responsible for making archive copies of all data tapes and
archiving them securely. In addition, user copies had to be made and
forwarded to the data representatives in the member countries. Copies of
Special Programme data collected during national experiments were only sent to
the respective member country, whereas all Common Programme data had to be
distributed to all member countries, requiring six copies. The copying and
archiving job was centralised to HQ in Kiruna, so tapes had to be physically
transported there as soon as convenient after an experiment. As shipments
from Tromsø and Sodankylä always involved a trip by car, a routine
soon developed where tapes were accumulated locally until the shipment could
be combined with a visit by a staff member for some other purpose. Sometimes
two, three or more boxfuls of tape were shipped at once, creating a massive
peak in the workload at HQ. Eventually a part-time data assistant position
with responsibility for all tape handling had to be created.</p>
      <p id="d1e760">After a few years, user demand and the availability of more computing power
in the form of the ND-530 machines led to the introduction of a
near-real-time quick-look analysis program, which produced first-order
estimates of standard parameters (plasma density, electron and ion
temperatures and velocities) on the fly. These estimates were also saved
and distributed to users. Following the installation of a ND-5400 machine in
1990, EISCAT HQ was connected to the Internet via the IRF and its
connections to SUNET, the Swedish university network. From this time
onwards, the physically small DAT and Exabyte tape formats were introduced
as a replacement for the reel-to-reel tapes, and data transfer and
distribution was gradually moved from physical media to file transfer over
the net, eventually replacing the shipping of raw data tapes from the sites
to HQ and putting an end to all shipping of tapes to the associates.</p>
</sec>
</sec>
<?pagebreak page15?><sec id="Ch1.S12">
  <label>12</label><title>Signal processing</title>
<sec id="Ch1.S12.SS1">
  <label>12.1</label><title>The Alker correlator</title>
      <p id="d1e779">The ultimate purpose of an incoherent scatter radar observing the ionosphere
is to determine the physical state of the scattering plasma: its electron
and ion temperatures, ion composition and bulk velocity. Any particular
combination of these parameters results in a corresponding distribution of
scatterer (electron) velocities, which in turn manifests itself as a
specific power frequency distribution of the scattered signal. After
processing by the radar receiver, the signal is sampled at regular time
intervals and digitised, such that the output from the ADC forms a
discrete time series of signal complex amplitude estimates. A
straightforward way to extract the desired information from the signal is
now to compute time-averaged autocorrelation functions (ACFs) over segments
of the sample stream. When EISCAT was in the planning stage, this
time-domain approach was already used at the Chatanika radar, where two
different digital correlators were in use, one hardwired for long pulse
modulations and the other semi-programmable (by rewiring) for multipulse
modulations. It was decided to follow this route also in EISCAT by employing
the famous “Alker correlator”.</p>
      <p id="d1e782">The Alker correlator promised to be a major improvement over the Chatanika
units. It started as a doctorate thesis project at the Norwegian technical
university in Trondheim (NTH), with design targets set by the envisaged
requirements of the coming EISCAT system and (at least initially) supervised
by Tor Hagfors. The result was a software-programmable device optimised for
computing complex-valued correlation functions, potentially very flexible
and in principle able to handle experiments combining several different
types of modulation in each radar cycle. A detailed description of its
pipelined architecture is given in Alker (1979). It was designed for a
sustained multiply–accumulate rate of 5 MHz, using the latest
state-of-the-art components, some of which were not even commercially
available as the work started: AMD 2900 bit-slice processors, TRW LSI <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:mn mathvariant="normal">8</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula> bit multiplier chips and static NMOS chips making up the input and output
memory banks. The program flow could be controlled by conditional jumping,
based on the values of three programmable loop counters, which allowed for a
degree of structured programming. Unfortunately, the program memory was only
63 instructions deep (it had to be very fast and was therefore expensive),
which was a severe limitation on an otherwise beautifully thought-out
design.</p>
      <p id="d1e797">The first physical realisation of the correlator turned out to be marginal.
It was constructed as two separate 19 in. rack-mounted units interconnected
by flat cables, one containing the double-banked input memory and the other
containing the arithmetic unit (the only part of that unit actually
constructed on printed circuit boards) and all control logic. The signal
ground provided by the flat-cable connection between the two units proved to
be too weak for the 5 MHz data rate. The ADCs used 2's complement data coding, so signal voltage variations around zero volts caused all data bits
on the bus to change from all zeros to all 1s or vice versa. Because of
the weak ground, this created lots of common-mode digital noise on the bus,
which partly corrupted the desired signal.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e803">The arithmetic unit of one of the Alker correlators. The front
panel layout has many features reminiscent of minicomputers of the 1970s
era, in particular the “data load” field with 16 switches to set up and
manually load individual micro-instructions into arbitrary program memory
locations; the front panel of the Nord-10 computer had an almost identical
field for the same purpose. Photo courtesy of Lars-Göran Vanhainen.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hgss.copernicus.org/articles/13/1/2022/hgss-13-1-2022-f07.jpg"/>

        </fig>

      <p id="d1e812">Internally, both the buffer memory unit and the computing unit were
constructed using wire-wrapping, a construction method extensively used for
logic systems in the 1970s and 1980s, which has now largely disappeared. It was
useful for producing prototypes or small series of non-standard systems, but
when improperly applied it could produce all sorts of illogical
malfunctions. Unfortunately, this was the case with the correlators. During
the first year of operation, the Kiruna unit could now and then stop in the
middle of an experiment and refuse to load and start, leaving the site staff
with no option other than to start pulling circuit boards. After a while, we
developed a very direct troubleshooting technique: the circuit boards were
banged down on the kitchen table, wire-wrap side down. This often caused one
or several pieces of overstretched and broken-off wrap wire to fall out of
the wire mat; it then remained to locate the broken connection and put in a
new wire!</p>
      <p id="d1e815">This unsatisfactory state of affairs could have continued for quite some
time, as there were only four correlators (three for the UHF system and one
for the VHF), and the demand for experiment operations was increasing all the
time, leaving no time for preventive maintenance. But in January 1983, a
capacitor in the Kiruna correlator exploded and set fire to some internal
cabling, spreading residue inside the unit and releasing acrid smoke that
triggered the fire extinguishing system. I was there when it happened. Fortunately, all<?pagebreak page16?> equipment was insured, and contact to the insurance
company confirmed that the repair costs would be reimbursed in full. A
rehabilitation programme was now started. All electronics in the receiver room
was thoroughly cleaned to prevent corrosion from the hydrochloric acid fumes.
At the same time, the VHF correlator was transferred from Tromsø to
Kiruna to allow tristatic measurements to continue; we could do this as the
VHF system had no transmitter at the time anyway. The burnt-out unit was
totally stripped out and rebuilt from the ground up by EISCAT staff, using
quality components and proper grounding techniques. Reliability improved
dramatically; the correlator could now operate for weeks on end without
stopping, and the common-mode noise in the data all but disappeared. The
other correlators were then rebuilt in the same way, one by one. By late
summer 1985 all four had been rebuilt. In the process, new result memory
boards were constructed, doubling the result memory space to 4096 addresses.
During 1986, a further improvement was introduced in the form of an internal
<inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">16</mml:mn></mml:mrow></mml:math></inline-formula> kiloword buffer memory. On a single circuit board, this provided twice the address space and all the functionality of the old buffer memory unit,
which became redundant and was removed. Once the rehabilitation programme had
been completed, the correlators behaved dependably and continued to do so
until being replaced by the new computer-based signal processing systems in
the early 2000s.</p>
</sec>
<sec id="Ch1.S12.SS2">
  <label>12.2</label><title>Correlation software – CORLAN and UNIPROG</title>
      <p id="d1e838">For the first few years, the correlator programmability was largely illusory
– programming still had to be done at the bit level, using a binary editor,
which made it a task for a very restricted group of specialists.
Accordingly, the first Common Programmes were built around a couple of the
basic algorithms originally developed by Alker for testing purposes, but the
inverse triangular lag weighting enforced by these made poor use of the
information contained in the scattered signal. To fully utilise the
frequency agility and modulation capabilities of the radar, a different,
more flexible approach to the signal processing task was needed.</p>
      <p id="d1e841">One path to this goal was to create a user-friendly, symbolic correlator
programming language, which would potentially make correlator programming
accessible to the community at large. After a couple of false starts and
unfinished attempts by different people, the Tromsø site programmer,
Bård Tørustad, finally managed to condense previous work in this
direction into a functioning assembly language, CORLAN, including a
cross-compiler written in Pascal (Tørustad, 1982).</p>
      <p id="d1e844">In parallel to this, Tauno Turunen and the Sodankylä site scientists
Markku Lehtinen and Johan Silén, in collaboration with expert programmer
Terrance Ho of the Max Planck Institute, developed a general purpose algorithm, UNIPROG, which was made available to the user community in 1983
(Ho et al., 1983).</p>
      <p id="d1e847"><?xmltex \hack{\newpage}?>UNIPROG was a decisive step forward. It introduced the concept of
visualising and organising the lagged products produced by the correlator
program as a triangular half matrix with all possible zero lags located on
the main diagonal and all other lag products located in the upper half, with
the non-zero lags located on successively shorter diagonals. Regardless of
the modulation used, be it long-pulse, multipulse, power profile or some
coded combination of these, the spatial resolution of an experiment could
then be selected by picking the desired number of points from each of these
diagonals. In this way, UNIPROG opened the possibility to combine up to
eight different modulations in the same experiment, limited only by the
computing speed (about 4 million multiply–accumulate operations per second max) and restricted result memory (initially only 2048 addresses) of the correlator.</p>
</sec>
<sec id="Ch1.S12.SS3">
  <label>12.3</label><title>The GEN system</title>
      <p id="d1e859">Turunen continued his quest for better utilisation of the available
information by combining the best features of UNIPROG and the flexibility
available through CORLAN into the GEN system (Turunen, 1986). This was a
fully developed set of correlator routines addressing what was arguably the
weakest point of the earlier processing algorithms, namely the bad spatial
and statistical weighting of the different lags in the monostatic long pulse
autocorrelation estimates. The improvement at lags longer than 50 <inline-formula><mml:math id="M24" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>s  was
dramatic, up to a factor 6 compared to the old CP-3. At the same time, total
power profile and multipulse processing flexibility was retained and the
background estimation improved.</p>
      <p id="d1e870">The GEN system library also included GEN-11, a very complex experiment
designed for D-region measurements. To achieve the desired <inline-formula><mml:math id="M25" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 1000 m
spatial resolution, GEN-11 employed phase coding of the basic pulse, using
the 13 bit Barker code decoders that had been part of the signal processing
chain from the start but only rarely used. Clutter cancellation was achieved
through an intricate pulse-to-pulse scheme, while lagged products were
computed out to 95 ms, thus meeting all reasonable demands for a
general purpose D-region code. Because of its complexity, GEN-11 was almost
never modified by users, but in unchanged form it was used as the core of
both Common and Special Programmes. The GEN system met with universal
acceptance, and before long, starting in 1985, GEN-type algorithms formed the
core of all Common Programmes.</p>
</sec>
<sec id="Ch1.S12.SS4">
  <label>12.4</label><title>Alternating codes and the alternating code decoder</title>
      <p id="d1e888">For some time it now appeared that the radar was being used almost to its
statistical limit – and this was indeed true as far as the “standard”
modulations went. But in parallel to Turunen's work, different forms of
power-domain coding had been studied by several authors and found promising,
particularly in high spatial resolution, low<?pagebreak page17?> signal-to-noise ratio
situations, for example, in the E layer at night, where they were expected to
outperform multipulse group codes by 2–4 times or more. Perhaps the most
well known were the so-called <italic>alternating codes</italic> (Lehtinen and Häggström, 1987), which
were derived from <italic>Walsh functions</italic> (see, for example, Wikipedia, <uri>https://en.wikipedia.org/wiki/Walsh_function</uri>, last access: 27 January 2022).</p>
      <p id="d1e900">Lehtinen, Häggström, Vallinkoski and coworkers tried alternating
codes on the UHF systems using UNIPROG to compute all lagged products of
the received samples from each code, dumping the intermediate, undecoded
results at brief intervals and performing the decoding offline after the
experiment. This approach worked and generated high-quality data, but it
also suffered from severe limitations, perhaps the worst of which was the
very restricted number of ranges that could be handled and the necessity to
use only 8 bit alternating codes; the limited result memory precluded using
the longer codes.</p>
      <p id="d1e903">It was clear that once the lessons from these first alternating codes
experiments had been absorbed by the user community, one could expect a
demand for the provision of user-friendly alternating codes capabilities at
both the UHF and the VHF, possibly followed by an upgrade of the Common
Programs. It was equally clear that the correlators were incapable of
handling this job as they stood. In simple terms, decoding an alternating
codes experiment reduces to computing a set of polynomials, where each term
in each polynomial is the product of an accumulated lagged product, fetched
from the result memory, and a sign bit generated from the code set. But when
the correlators were designed in the late 1970s, the need for this type of
operation was not anticipated, and so the only arithmetic function
implemented on the result memory side was straightforward accumulation.</p>
      <p id="d1e906">We were thus faced with a choice: either replacing the correlators with high
performance workstations, which were only then becoming available, or
accepting the challenge of somehow modifying the correlators to enable
on-the-fly decoding of alternating codes, while leaving all other functions
intact. After careful weighing of the pros and cons, the second alternative
won out; it would allow UNIPROG- and GEN-system-based experiments to run as
before, almost transparently, while at the same time avoiding the
uncertainties, development work and extra costs associated with porting the
signal processing task to new, unfamiliar hard- and software systems.</p>
      <p id="d1e910">After quite a bit of thinking, a solution to the decoding problem was found,
using a previously unused data port into the correlator arithmetic unit to
interface a newly designed sign bit generator–multiplier unit between the
buffer memory and the correlator arithmetic unit. The concept was worked
out, prototyped and tested in the Kiruna correlator. Once found working as
planned, the added functionality was made accessible to users through a
special driver, ALTCODE, which was added to the GEN system library. Decoders
were eventually installed in all correlators, and a “second-generation”
programming environment, G2, combining the GEN system and the alternating
code capability, was developed and published (Wannberg, 1993).
G2-experiments were first used in regular scientific experiments in late
1990 with good results. Next, CP-1K, a new version of Common Programme CP-1
(see below), was developed, where the interlaced multipulses of the previous
version were replaced by a 16 Bd alternating code modulation. The same
modulation pattern was also soon introduced into CP-2, yielding considerably
improved performance in low signal-to-noise conditions. After these
developments, the signal processing hardware was essentially left untouched
and performed well for a decade, until finally replaced by a system
patterned on the one developed for the EISCAT Svalbard radar.</p>
</sec>
<sec id="Ch1.S12.SS5">
  <label>12.5</label><title>Common Programmes</title>
      <p id="d1e922">Throughout the first 2 decades, the Common Programmes continued to meet the
basic concepts drawn up at the outset as far as their areas of coverage were
concerned, in agreement with the idea to generate a database covering as
long a time span as possible – but their performance increased all the time
thanks to the improvements on the signal processing side. CPs 1, 2 and 3
were UHF experiments. CP-1 was a field-aligned experiment with altitude
coverage to above 600 km, tristatic velocity measurements in the F region
and kilometre-scale altitude resolution in the E region, and CP-2 was essentially the
same experiment, but scanning through four closely spaced beam directions
enclosing the Tromsø field line. CP-3 implemented an F-region latitude
scan covering the entire common field of view of the UHF system. CP-4 was a
derivative of the British Polar experiments, using the VHF in dual beam mode
to measure the plasma velocity field to the north of Tromsø to Svalbard
and beyond. CP-6 was used for high resolution measurements in the E and D
regions, and CP-7 was a dedicated high-altitude VHF experiment. The modulations
used were essentially variants of Turunen's GEN programmes or (in the case of
CP-1 and 2) copies of CP-1-K and remained basically unchanged until the
signal processing system was replaced, starting around y2000.</p>
</sec>
</sec>
<sec id="Ch1.S13">
  <label>13</label><title>Timekeeping and frequency keeping</title>
      <p id="d1e934">Operating the tristatic UHF with pulsed transmissions, instead of with CW,
required very precise relative timekeeping between the three sites. With
the most probable pulse lengths being in the 300–400 <inline-formula><mml:math id="M26" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>s  range, a relative
clock drift of at most some 5 % or 15–20 <inline-formula><mml:math id="M27" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>s would be tolerable. This
was doable, but not simple, in the 1970s – this was long before the time of
GPS and other satellite-borne systems distributing reference time and
frequency, and so the only way to guarantee this level of accuracy over any
reasonable length of time was by having Cs beam clocks at all sites.</p>
      <?pagebreak page18?><p id="d1e953">A typical Cs beam clock is expected to drift by less than <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">12</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>  relative to
an ensemble of similar clocks. This translates to a little less than
one-tenth of a microsecond per day, so with three well-behaved clocks, one
could expect the system to stay in time for about a hundred days or more,
once the clocks had been set to a common reference, the “master clock”.
This was a fourth, battery-operated Cs clock that could be transported
between the sites by car. Clock transports typically happened about once a
year or whenever the signals received at Kiruna and/or Sodankylä started
to drift out of the expected reception windows.</p>
      <p id="d1e974">The Cs clocks also generated an extremely stable 5 MHz frequency reference
signal, which was used to phase-lock all oscillators in the transmitter and
receiver systems. In this way the relative TX-to-RX frequency uncertainty at
933 MHz was less than <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> Hz, negligible compared to the <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> Hz
residual shift of the transmitted frequency caused by klystron phase pushing
during the pulse.</p>
      <p id="d1e1007">However, the Cs clocks lacked a very important feature – while they
generated an extremely accurate train of 1 s<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> pulses, able to be set to better than
a microsecond, they had no built-in machine-readable time output port. To
remedy this, EISCAT staff designed and constructed a real-time clock (RTC).
Controlled by the 1 s<inline-formula><mml:math id="M32" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> ticks from the Cs clock, this unit provided both a
time display and a time output port. It also generated start pulses for
various time-critical subsystems, primarily the radar controller unit. For
this purpose it was fitted with a programmable delay register that could be
loaded from the system computer.</p>
      <p id="d1e1035">As an extra fallback, each site also had a Loran-C receiver tuned to the
Loran-C transmitter at Bø in Vesterålen, which transmitted an
extremely precise Cs-clock-controlled signal at 100 kHz. Special receivers
comparing the local clocks against the sync pulses transmitted by the
Yllästunturi TV transmitter were also used to monitor the relative drift
of the Kiruna and Sodankylä clocks.</p>
      <p id="d1e1038">To facilitate global experiment control and data analysis and archiving, the
site clocks had to be synchronised to universal time (UTC). From time to
time, the master clock was therefore transported to the Swedish national
time and frequency standard, a pool of high-performance Cs clocks maintained
at the Swedish defence research establishment (FOA) in Stockholm and there
reset to UTC to the nearest microsecond. The transport was normally effected
by booking two tickets on a regular flight from Kiruna to Stockholm, one for
the clock and one for the timing engineer, and seating the clock in its
booked aircraft seat, a procedure which would be unlikely to be allowed
now. As an amusing aside, on one occasion during the “technical period”,
the travelling clock was flown from Kiruna to Sodankylä in a small
private seaplane piloted by the then assistant director science, who held a
private pilot license. The plane landed on the Kitinen River, next to the
EISCAT site, only to be immediately inspected by two serious customs
officials who had been ordered there for the occasion.</p>
      <p id="d1e1041">Part way into the construction period, it was realised that making all three
UHF antennas steerable added a new degree of complexity to the timing
system. Since the tristatic intersection point could now be anywhere in the
common field of view of the three sites, the time between the transmission
of a pulse from Tromsø and the arrival of the scattered signal at a
remote site could be anything from about 600 <inline-formula><mml:math id="M33" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>s to 20 ms – but the
reception window at the remote sites could only be made about a millisecond
long due to the limitations imposed by the correlator.</p>
      <p id="d1e1052">An elegant combination of hardware and software resolved this issue.
Whenever an antenna-pointing command was executed at a remote site, the
propagation time from Tromsø to the beam intersection point and thence to
the receiver was automatically computed by an EROS operating system routine
and loaded into the RTC delay register. The RTC then delayed the start pulse
to the ADCs by this amount, thereby making the signal always appear at the
same relative point in the sample vector and relieving users from having to
compute and program timing details in advance.</p>
</sec>
<sec id="Ch1.S14">
  <label>14</label><title>Frequency spectrum issues</title>
      <p id="d1e1063">Dictated by the plasma physics of the ionosphere, the optimal operating
frequencies of incoherent scatter systems lie in the VHF–low UHF region,
approximately 50–1000 MHz, the VHF frequencies being most suitable for low
electron density conditions. To maximise the scientific returns from the
EISCAT system over the whole 75–2000 km altitude range, the plan was
therefore to obtain a UHF allocation just below 1000 MHz and a VHF
allocation at approximately 240 MHz (du Castel et al., 1971). Also, to
achieve the full potential of the project, access to up to 30 MHz of
interference-free spectrum centred on the allocated operating frequencies
was desired; only in this way would it be possible to employ frequency-hopping in
order to use the full 12.5 % transmitter duty cycle and simultaneously
receive both up- and downshifted plasma line returns.</p>
      <p id="d1e1066">Unfortunately, most of the 50–1000 MHz range is allocated to a great
number of active services (FM broadcasting, TV, mobile phone systems, etc.) and
heavily congested everywhere, also in Scandinavia. The EISCAT allocations
therefore had to be fitted into already established frequency plans on a
mutual non-interference basis without deviating too much from the initial
targets.</p>
      <p id="d1e1069">In the late 1970s, this was still possible. VHF TV channel 12 was not used in
northern Norway, which left a convenient spectrum slot for a VHF system
between 222.75 and 230.0 MHz. A transmitting permit for <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mn mathvariant="normal">224</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:math></inline-formula> MHz
was applied for from the Norwegian P&amp;T (NPT) at an early stage and duly
issued. This allocation proved to be fairly unproblematic; some
interference, probably emanating from TV transmitters farther south, could
be observed from time to time but did not seriously upset the VHF
observations.</p>
      <?pagebreak page19?><p id="d1e1084"><?xmltex \hack{\newpage}?>For the UHF, an allocation at about 930 MHz was desirable, based on
experience from the French St. Santin system. This also appeared possible,
as the 918–948 MHz frequency band was not used by any radio services in
Norway, nor in Sweden or Finland. Nevertheless, the band could not be
allocated to EISCAT on a protected basis because in the ITU region 1
frequency plan, first priority to its use was given to “fixed-to-mobile
communications”, that is, mobile phone systems. In Sweden, a pure receiver
system like the Kiruna UHF station did not require any special permit. On
the other hand, Swedish telecom law did not provide any mechanism for
granting interference protection to a receiver site. Rules in Finland were
similar. But at this point in time, no collision of interests was foreseen;
the EISCAT project was expected to last for about 13 years and terminate
well before any mobile networks would be deployed in northern Scandinavia.
On this assumption, a transmitting permit for <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mn mathvariant="normal">933.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> MHz was issued
by the NPT, the UHF system was set up accordingly and the community looked
forward to many years of undisturbed wideband operation.</p>
      <p id="d1e1101">But reality proved to be different; the initially promising spectrum
situation soon developed into an existential threat to the whole UHF system.
A new mobile phone service using the 935–942.5 MHz band, NMT900, was already
introduced in the metropolitan areas of all Nordic countries in
December 1986. It rapidly expanded northwards and reached Kiruna in early
1988. The NMT900 base station signals immediately drove the Kiruna receiver
into non-linearity, even though they were outside the EISCAT band. To rescue
the continued operation, the UHF receiver front ends had to be completely
redesigned and rebuilt to increase their dynamic range, the UHF transmitter
frequency band was downshifted by 2 MHz (the limit of what the klystron
could handle) and agreements were reached with the NMT operators in all
three host countries to restrict the NMT900 base stations near the EISCAT
sites to transmit only above 939 MHz. It was only by August 1990 that these
actions finally enabled the UHF to return to routine tristatic ion line
operation, but plasma line observation possibilities had now become severely
restricted in the process.</p>
      <p id="d1e1104">However, the EISCAT interplanetary scintillation (IPS) programme was badly
affected. Being a passive technique, IPS requires access to wide segments of
interference-free spectrum to obtain statistics, a feature it shares with
radio astronomy observations. At EISCAT, the IPS groups had until then been
able to use the full available UHF bandwidth, 30 MHz, but now became
restricted to 8 MHz or less; further bandwidth cuts in the future could not
be ruled out. An in-house development programme was therefore started with the
goal of establishing receiving capabilities in the 1410–1427 MHz protected
radio astronomy band at Kiruna and Sodankylä. When completed, the 1400 MHz system performance matched the best previous 933 MHz results and gave
the IPS programme an extra 10 years.</p>
      <p id="d1e1107">In an effort to obtain support for EISCAT's continued need for undisturbed
spectrum, HQ contacted CRAF, the Committee for protection of Radio Astronomy
Frequencies, a sub-committee of the European Science Foundation charged with
safeguarding radio astronomy and remote-sensing frequency bands and
combating spectrum pollution. While protection of active radar operation did
not fall within the purview of CRAF, safeguarding the IPS and other passive
observations at EISCAT was seen as having sufficient merit to warrant
admitting EISCAT to the committee. First admitted with observer status,
EISCAT eventually gained full membership. From the early 1990s until 2012, I
served as the EISCAT delegate. The CRAF meetings were a very useful
clearing house for news about the spectrum situation in Europe and potential
threats to all radio-based observation activities and also offered an
excellent channel for establishing awareness and understanding of EISCAT in
the radio astronomy community.</p>
      <p id="d1e1110">In 1998, the association's initially planned-for 13 years of operation had
come to an end, but the system was generating very good science, and users
and owners both wished to continue the operation. This required an extension
of the transmitting permits. Negotiations with the NPT followed, and in 1989
an extension was granted, this time however with the proviso that the
situation should be re-evaluated every other year. A little later, a new
digital mobile phone service (GSM) was introduced all over the Nordic
countries. Thanks to the excellent cooperation with the national spectrum
management authorities established in the aftermath of the NMT900 problems,
this did not at first cause major interference problems, but in 2005 the
Sodankylä UHF receiver was swamped with wideband interference. A new GSM
operator had unwittingly set up its base stations in the town of Sodankylä to
transmit in the 929.0–935.0 MHz range, which was protected under an
agreement between EISCAT and the Finnish P&amp;T. The operator was approached
and rapidly reprogrammed all stations, which eliminated the worst
interference. Unfortunately, transmissions in this frequency range
originating from other base stations more than 100 km away still affected
reception in certain directions at low antenna elevations. As yet more
networks were established in the area, the useable Sodankylä receiving
band shrank further and eventually became restricted to just 929.0–931.5 MHz, a dramatic deterioration from the 1980s situation.</p>
      <?pagebreak page20?><p id="d1e1113">These problems notwithstanding, routine UHF ion line operations continued
for more than another decade. By 2010, EISCAT had operated for 29 years,
more than twice the originally foreseen lifetime of the association, and the
mainland system was still providing valuable data. But this year, Sweden and
Finland were obliged to ratify a EU directive to open the 900 MHz band to
third-generation digital mobile phone services, UMTS 900. When this new service
started up in the vicinity of the Kiruna and Sodankylä sites in 2011,
their remaining UHF spectrum windows were immediately blanked out by
wideband interference. Thus, after 30 years of operation, the world's
only tristatic ISR system was effectively reduced to a monostatic radar, and
its unique vector data capability was lost, possibly for good. But a partial
remedy was found and implemented: in 2012 the remote UHF dishes were adapted
for VHF reception by replacing the subreflectors with prime-focus feeds,
following a proposal by the IRF EISCAT group (Wannberg, 2010). On 1 November 2012, the very first tristatic VHF experiment was successfully run. In
this way, tristatic EISCAT gained a respite, albeit in a restricted
geometry, the VHF beam being limited to pointing vertically. The system is
still occasionally run in this configuration as this is being written.</p>
</sec>
<sec id="Ch1.S15" sec-type="conclusions">
  <label>15</label><title>Personal reflections</title>
      <p id="d1e1124">My background and route into EISCAT were quite different from most of my
colleagues. In 1979, on completing my Ph.D. in nuclear physics at Uppsala
University, I started to look for a job. At about this time, EISCAT HQ was
advertising in major Swedish newspapers. The EISCAT project looked very
technically attractive, and I felt that maybe it could use me somehow; I had
been trained as an experimentalist, much of my work had been performed in an
international environment at CERN, our system contained a great deal of
radio frequency technology and I was also an enthusiastic radio amateur
who once dreamt of getting into radio astronomy professionally.</p>
      <p id="d1e1127">That spring, I applied for a scientific programmer position at HQ, was
interviewed and turned down – but a few weeks later I got a phone call out
of the blue from the Swedish Institute of Space Physics. They had got hold
of my application to EISCAT and liked it, I was invited to an interview
and the next day I was offered a research engineer position in the satellite
group! I jumped at the opportunity and started on the job in November 1979,
spending the first couple of months studying up on plasma physics, but all
the time I kept an eye out for any opportunities at EISCAT. When the Kiruna
site manager position was about to become vacant in 1981, I applied for it
and got it, perhaps because I was the only applicant – Hultqvist
regarded my choice as a voluntary demotion!</p>
      <p id="d1e1130">Taking up my new position in June 1981, I was still a green newcomer to the
geophysics community and my understanding of the scientific tasks that the
founding fathers of EISCAT and the associate scientists had set for
themselves was almost nil. In a way, the whole time from then until I
departed EISCAT in 2008 came to be a continuous learning-on-the-job process,
apparently with some success; in 1987 I was recruited by Jürgen Röttger to fill the HQ position of assistant director (technique) and
later promoted to deputy director, a position I held until my departure. My
contributions to the development of the radar system peaked during the
Svalbard radar project and culminated in my leading the
EISCAT_3D feasibility study. I always regarded my role in
EISCAT as that of a <italic>machine physicist</italic>, a concept I learned of at CERN, but I am happy that in
helping to introduce the study of meteor head echoes with the UHF system I
was also able to do a bit of science with the instrument. I am extremely
grateful that I was able to join the EISCAT community right at the beginning
of the operational phase and given the opportunity to help developing and
steering the radar system through a period that was arguably its best years,
when the VHF and UHF spectrum windows were still wide open, new and
unexpected results were emerging regularly and coding and signal processing
theory and technology made great advances.</p>
      <p id="d1e1136">Today, more than 45 years after the inception of the EISCAT Kiruna–Sodankylä–Tromsø (KST), its
successor, EISCAT_3D, is faced with a whole new situation.
Solid-state technology has advanced to the point where phased-array systems
with thousands of individually driven elements are now the obvious choice
for new radar systems, and computational power many orders of magnitude
larger than that of the EISCAT correlators is available in every laptop,
thus trivialising the signal processing task. But at the same time, the
explosive growth of digital mobile phone systems and the transition from analogue
to digital TV broadcasting has caused a massive demand for low UHF spectrum,
leaving almost no holes below 1 GHz. Protected, undisturbed access to
frequency bands wide enough to cover the whole scatter spectrum can no
longer be had in developed areas, for example, northern Scandinavia, and no help
is to be expected from the radio astronomy community, which regards any
transmission as anathema. It was only with difficulty that a slot at 233 MHz
could be identified and accepted by the Norwegian spectrum management
authority as suitable for the active part of EISCAT_3D.
Neighbouring bands are filled with digital audio broadcasting signals, some
of which will spill over into the radar band and increase the noise level
there, which is likely to make plasma line reception hard or maybe even
impossible. The proliferation of consumer electronics has also made the
general interference situation much worse. One can only hope that advanced
coding and signal processing can help out.</p>
      <p id="d1e1140">I fondly remember the simpler times of the 1980s and 1990s and wish the new
generation the best of luck in meeting today's and tomorrow's challenges.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e1147">No data sets were used in this paper. All citations appear in the reference list.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e1154">The contact author has declared that there are no competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e1160">Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><notes notes-type="sistatement"><title>Special issue statement</title>

      <p id="d1e1166">This article is part of the special issue “The history of ionospheric radars”. It is not associated with a conference.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e1172">Ingemar Wolf and Lars-Göran Vanhainen, two colleagues from my time at
the Kiruna site who both started with EISCAT before myself – Ingemar was
actually working in the project from the very beginning in 1976 – have
generously shared their own recollections of the early times. Mike Rietveld
kindly provided photos of the capacitor bank and the crowbar.
Thanks are given to the referees for valuable corrections and comments.</p></ack><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e1177">This paper was edited by Kristian Schlegel and reviewed by Michael Rietveld and Philip Erickson.</p>
  </notes><ref-list>
    <title>References</title>

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Baron, M.: EISCAT progress 1983–1985,  J. Atmos. Terr. Phys., 48, 767–772, 1986.</mixed-citation></ref>
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Willis, D. M., Crothers, S. R., Todd, H., and Cowley, S. W. H.: Scattered power
from non-thermal, F-region plasma observed by EISCAT – evidence for
coherent echoes?, J. Atmos. Terr. Phys., 50, 467–485, 1988</mixed-citation></ref>
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McKay-Bukowski, D., Vierinen, J., Virtanen, I., Fallows, R., Postila, M.,
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Gerbers, M., Grit, T., Gruppen, P., Kero, A., Iinatti, T., Lehtinen, M.,
Meulman, H., Norden, M., Orispää, M., Raita, T., de Reijer, J. P.,
Roininen, L., Schoenmakers, A., Stuurwold, K., and Turunen, E.: KAIRA: The
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Röttger, J., La Hoz, C., Kelley, M. C., Hoppe, U.-P., and Hall, C.:  The
structure and dynamics of polar mesosphere summer echoes observed with the
EISCAT 224 MHz radar, Geophys. Res. Lett., 15, 1353–1356, 1988</mixed-citation></ref>
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Tørustad, B. W.: CORLAN (COrrelator LANguage), EISCAT Technical Note,
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Turunen, T.: GEN-SYSTEM – a new experimental philosophy for EISCAT radars,
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      <ref id="bib1.bib21"><label>21</label><?label 1?><mixed-citation>
Turunen, T., Mustonen, T., and Williams, P.: EISCAT UHF Receivers: Report and
recommendations, EISCAT Technical Note, .SOC6, Swedish Institute of Space Physics, 2010, unpublished, 1981.</mixed-citation></ref>
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Wannberg, G.: The G2-system and general purpose alternating code experiments
for EISCAT, J. Atmos. Terr. Phys., 55, 543–557, 1993.</mixed-citation></ref>
      <ref id="bib1.bib23"><label>23</label><?label 1?><mixed-citation>
Wannberg, G.: Proposal from the IRF-K EISCAT User Groups: Saving EISCAT's
vector velocity and E field measurement capabilities by converting the
Kiruna and Sodankyla' 32-m UHF antennas to VHF operation,
document tabled at SOC 6,  unpublished, 2010.</mixed-citation></ref>
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Eliassen, S., Heck, S., and Huuskonen, A.: The ElSCAT Svalbard radar: A case
study in modern incoherent scatter radar system design, Radio Sci., 32,
2283–2307, <ext-link xlink:href="https://doi.org/10.1029/97RS01803" ext-link-type="DOI">10.1029/97RS01803</ext-link>, 1997.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>History of EISCAT – Part 5: Operation and development of the system during the first 2 decades</article-title-html>
<abstract-html/>
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Alker, H. J.: A Programmable Digital Correlator Module for the EISCAT Radar
System, EISCAT Technical Note, 79/11, 1979.
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<ref-html id="bib1.bib2"><label>2</label><mixed-citation>
Armstrong, J.: EISCAT Experiment Preparation Manual, EISCAT Technical Note,
80/22, 1980.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation>
Baron, M.: EISCAT progress 1983–1985,  J. Atmos. Terr. Phys., 48, 767–772, 1986.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation>
Bauer, P., Giraud, A., Kofman, W., Petit, M., and Waldteufel, P.: How the Saint Santin incoherent scatter system paved the way for a French involvement in EISCAT, Hist. Geo Space. Sci., 4, 97–103, <a href="https://doi.org/10.5194/hgss-4-97-2013" target="_blank">https://doi.org/10.5194/hgss-4-97-2013</a>, 2013.
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<ref-html id="bib1.bib5"><label>5</label><mixed-citation>
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Incoherent Scatter Facility in the Auroral Zone (EISCAT),
Auroral Observatory, Tromsø,  June 1971.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>6</label><mixed-citation>
Farmer, A.: EISCAT Data Gathering and Dissemination, published by EISCAT Technical Note,
80/23, 1980.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>7</label><mixed-citation>
Haerendel, G.: History of EISCAT – Part 4: On the German contribution to the early years of EISCAT, Hist. Geo Space. Sci., 7, 67–72, <a href="https://doi.org/10.5194/hgss-7-67-2016" target="_blank">https://doi.org/10.5194/hgss-7-67-2016</a>, 2016.
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Horner, F., Kohl, H., Oksman, J., Ranta, O., Sandbo, A., Schneider, F., and
Wilhelmsson, H.: A European Incoherent Scatter Facility in the Auroral Zone,
Organization and Operation, Implementation of the UHF part of the System,
presented by the EISCAT Steering Committee,  Trondheim, June 1974.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>9</label><mixed-citation>
Ho, T., Turunen, T., Silén, J., and Lehtinen, M.: The Lag Profile Routine
and the Universal Program for the EISCAT Digital Correlators, EISCAT
Technical Note, 83/37,  1983.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>10</label><mixed-citation>
Holt, O.: History of EISCAT – Part 3: The early history of EISCAT in Norway, Hist. Geo Space. Sci., 3, 47–52, <a href="https://doi.org/10.5194/hgss-3-47-2012" target="_blank">https://doi.org/10.5194/hgss-3-47-2012</a>, 2012.
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Hultqvist, B.: History of EISCAT – Part 1: On the early history of EISCAT with special reference to the Swedish part of it, Hist. Geo Space. Sci., 2, 115–121, <a href="https://doi.org/10.5194/hgss-2-115-2011" target="_blank">https://doi.org/10.5194/hgss-2-115-2011</a>, 2011.

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station at the Russian Polar Geophysical Institute, the current status and a
brief description,  J. Atmos. Terr. Phys.,  55,  559–556, 1993.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>13</label><mixed-citation>
Lehtinen, M. S. and Häggström, I.: A new modulation principle for
incoherent scatter measurements, Radio Sci., 22, 625–634,
<a href="https://doi.org/10.1029/rs022i004p00625" target="_blank">https://doi.org/10.1029/rs022i004p00625</a>, 1987.
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Willis, D. M., Crothers, S. R., Todd, H., and Cowley, S. W. H.: Scattered power
from non-thermal, F-region plasma observed by EISCAT – evidence for
coherent echoes?, J. Atmos. Terr. Phys., 50, 467–485, 1988
</mixed-citation></ref-html>
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McKay-Bukowski, D., Vierinen, J., Virtanen, I., Fallows, R., Postila, M.,
Ulich, T., Wucknitz, O., Brentjens, M., Ebbendorf, N., Enell, C.-F.,
Gerbers, M., Grit, T., Gruppen, P., Kero, A., Iinatti, T., Lehtinen, M.,
Meulman, H., Norden, M., Orispää, M., Raita, T., de Reijer, J. P.,
Roininen, L., Schoenmakers, A., Stuurwold, K., and Turunen, E.: KAIRA: The
Kilpisjärvi Atmospheric Imaging Receiver Array – System Overview and
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2015
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Oksman, J.: History of EISCAT – Part 2: The early history of EISCAT in
Finland, Hist. Geo Space. Sci., 2, 123–128, <a href="https://doi.org/10.5194/hgss-2-123-2011" target="_blank">https://doi.org/10.5194/hgss-2-123-2011</a>,
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Röttger, J., La Hoz, C., Kelley, M. C., Hoppe, U.-P., and Hall, C.:  The
structure and dynamics of polar mesosphere summer echoes observed with the
EISCAT 224&thinsp;MHz radar, Geophys. Res. Lett., 15, 1353–1356, 1988
</mixed-citation></ref-html>
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Tørustad, B. W.: CORLAN (COrrelator LANguage), EISCAT Technical Note,
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Turunen, T.: GEN-SYSTEM – a new experimental philosophy for EISCAT radars,
J. Atmos. Terr. Phys., 48,  777–786, 1986.
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Turunen, T., Mustonen, T., and Williams, P.: EISCAT UHF Receivers: Report and
recommendations, EISCAT Technical Note, .SOC6, Swedish Institute of Space Physics, 2010, unpublished, 1981.
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Eliassen, S., Heck, S., and Huuskonen, A.: The ElSCAT Svalbard radar: A case
study in modern incoherent scatter radar system design, Radio Sci., 32,
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</mixed-citation></ref-html>--></article>
