IRI/COST Workshop, Prague, Czech Republic, July 10-14, 2007
Ionosphere –
Modelling, Forcing, and Telecommunications
Dieter Bilitza
The workshop continued the bi-annual meetings
that the COSPAR/URSI Working Group on the International Reference Ionosphere
(IRI) organizes in years between the COSPAR General Assemblies. These workshops
are the prime venue for discussions of model shortcomings, improvements, new
model additions, applications, and other IRI-related topics. These meetings
have grown from small gatherings of experts to well-attended workshops with a
good representation of the many countries involved in the IRI effort and a good
balance between the different measurement techniques that are contributing to
the IRI success. For the Prague Workshop the IRI team joined forces with the
European Cooperation for the Mitigation of Ionospheric Effects on Radio Systems
(COST 296) one of the major pan-European projects in ionospheric physics supported
by the European Cooperation in the Field of Scientific and Technical Research
(COST). The special focus of this combined IRI/COST workshop was a better
representation of the forcing from below and from above in ionospheric models
with special emphasis on the IRI model and regional European models. Naturally
the workshop had a strong orientation towards application of ionospheric models
and specifically on their effects on radio systems. The meeting was expertly
organized by the Local Organizing Committee (Lastovicka, Buresova, Sauli,
Truhlik, Triskova) whose untiring effort not only made this a very productive
meeting but also a memorable time for everybody in the Golden City including an
excursion to the beautiful Konopiste Castle.
The
workshop was attended by 103 participants from Africa, Asia, Europe, and North
and South America. 67 oral and 50 poster papers were presented. The agenda
included sessions on Ionospheric Effects on Radio Systems, GPS and TEC,
Topside, Ionospheric Storm Effects, Ionospheric Sounding, F Peak Mapping,
Bottomside and E-Region, the IRI Final Discussions, and the COST296 Management
Committee meeting. Papers and posters from the meeting will be considered for a
special issue of Advances in Space Research.
The
meeting was financially supported by COSPAR, URSI, IAGA, the European Office of
Aerospace Research & Development (EOARD) of the US Air Force, the US Office
of Naval Research (ONR), and the Czech Academy of Sciences, providing travel
funds (full or partial) for 14 scientists from Argentina, China, Georgia,
India, Iraq, and Turkey.
F-PEAK MAPPING
Increased accuracy of models for the F-peak
parameters (foF2, NmF2, hmF2, M(3000)F2) is an important goal of both IRI and
COST. COST is primarily focussed on the European sector while IRI has to deal
with the whole globe. Several modelling approaches were presented including
Neural Networks (NN) (Yu, China; Y. Tulunay, Turkey; Habarulema, South Africa;
Tomasik, Poland), Genetic Algorithms (F. Arikan, Turkey), Eigen-mode Analysis
(Wan, China) and others. Very promising are NN models for foF2 and M(3000)F2
developed by McKinnell et al. (South Africa) that are trained with a large
volume of ionosonde data. Comparisons with data not used in the training
process show significant improvements versus the older CCIR and URSI models. It
was decided to include their M(3000)F2 model in the next version of IRI to get
a better representation of the hmF2 evening peak; the peak height hmF2 is
correlated with the propagation factor M(3000)F3 that is routinely scaled from
ionograms. More work is still
needed for the foF2 model in particular a more globally homogenous data base
including data from more ionosondes (e.g., Brazilian and Chinese ionosondes are
currently not included) and from topside sounder satellites. An important
outcome of the Prague meeting is the forming of a special task group on F-peak
mapping to bring together data providers and modellers and to facilitate
inclusion of the improved models in IRI and in operational programs. The task
group includes members from IRI and COST and is led by Bilitza (USA). A first
task is to interact with the International Telecommunication Union
-Radiocommunication (ITU-R) group whose proposal is to digitise the existing CCIR maps on a 2.5 degree
latitude/longitude grid and to publish new maps every 5 years (Bradley, USA).
TOPSIDE AND TEC
Many of the GNSS-related presentations
discussed the deduction of peak and profile information from the slant path
phase and amplitude measurements using simple profile assumption or a more
sophisticated tomographic approach. Difficulties remain in areas of large
ionospheric gradients and/or scarce ground station coverage and also because of
insufficient knowledge of the plasmaspheric contribution. The new constellation
of COSMIC satellites carrying GPS receivers into space helps to overcome some
of the coverage problems but has to deal with the inherent limitations of the
radio occultation technique. Comparisons with Jicamarca incoherent scatter
radar and ionosonde measurements, for example, showed that assimilating COSMIC
and GPS data into the JPL/GAIM model led to improvements in the topside, but
made results worse in the F layer (Rich, USA). Several presentations showed how
using IRI as an a priori source of information, can lead to improvements in the
tomographic construction of 3-D maps (O. Arikan, Turkey; Zeilhofer, Germany;
Bhuyan, India). Good progress is made in accounting for higher order
ionospheric effects (Hernandez-Pajares, Spain) and significant improvements are
expected from the third frequency that will be standard with the European
Galileo system (Spits, Belgium).
IRI-2007
offers two new options for the topside electron density profile: NeQuick and a
corrected IRI-2001. First evaluations of these new additions were inconclusive:
A comparison with Alouette/ISIS topside sounder data favored the NeQuick option
(Bilitza, USA) whereas an analysis with CHAMP and COSMIC data finds better
agreement with the corrected IRI-2001 option (Mayer, Germany). IRI-2001-corr
seems to include a more accurate representation of the spatial and altitudinal
structure of the Equator Anomaly while IRI-NeQuick scores higher when data from
all latitudes are considered. NeQuick
was also compared with GNSS data in China (J. Shi, China) and Europe (Bedaine,
Belgium) and with regional models based on these data. Measurements from the
Indian SROSS C2 satellite at ~500 km illustrate the close coupling of EA
parameters with the equatorial electrojet (Bhuyan, India) and might help in
further evaluating the two different options.
An important parameter for the
representation of the topside electron density profile is the ionospheric scale
height. Besides the standard plasma scale height that varies from an Oxygen
scale height near the peak to a light ion scale height higher up, modelling
often relies on the Òvertical scale heightÓ assuming an exponentially decaying
profile or an Òeffective scale heightÓ assuming a Chapman-type profile (L. Liu,
China). Global models for this scale height and its variation with altitude are
an area of study of several IRI and COST researchers presenting progress
reports at this meeting (Kutiev, Bulgaria).
BOTTOMSIDE
Comparisons of ionosonde (McKinnell, South
Africa) and incoherent scatter radar data with IRI illustrated the shortcomings
of the current tabular form of the representation of annual and global
variations of the bottomside profile parameters (B0, B1, D1). The spherical
harmonics approach by Altadill and Blanch (Spain) showed much better results
and will be included in the next version of IRI.
The representation of ionospheric
storm effects in IRI is currently limited to the F-peak density and IRI represents
quite well the mostly negative ionospheric storm effects observed in
mid-latitude summer (Buresova, Czech Republic). Inclusion of the storm-induced uplift
of the layer (Reinisch, USA) is a high priority goal for future versions of
IRI. A new effort is looking at a model description of E-region effects using
more than 6 years of TIMED/SABER NO+(v) 4.3 μm Volume
Emission Rate (VER) data, an
excellent proxy for studying E-region chemistry (Mertens, USA).
PLASMA TEMPERATURES AND ION DRIFT
In the area of plasma temperatures accurate representation of solar cycle effects is a top priority. When combining incoherent scatter radar and DMSP satellite data towards this goal, significant discrepancies were found between the ground and space measurements at low solar activities, likely due to the low electron densities which make accurate electron temperature determination in the topside ionosphere difficult for both techniques. At lower altitudes a large database of satellite in situ measurements is being used to establish the average variation patterns of Te over the solar cycle for different local time, season, and latitude (Truhlik et al., Czech Republic).
The new equatorial zonal drift
model of Fejer et al. (USA) based on Jicamarca incoherent scatter radar
measurements was proposed for IRI and will be included in the next version
complementing the already included vertical drift models by the same authors. The
model includes dependences with solar activity and season and reproduces the
observed westward daytime drifts and eastward nighttime drifts. A study of
magnetic storm effects on the ion drift based on observations with the
Pruhonice, Czech Republic digisonde shows dramatic increases in E and F region
drifts at this mid-latitude station (Boska, Czech Republic). S.-Y. Su (Taiwan)
used ROCSAT data to study the occurrence statistics of equatorial density irregularities
and their correlation with vertical drift velocities
NEW INPUTS FOR IRI
Many of the COST-296-specific
topics are also of great interest for IRI. A series of presentations reviewed the status and progress of
these activities including HF communications (airplane, ship, HF radar,
military; circuit diagnostics, frequency management), ionospheric
scintillations, and ionospheric influence on performance of various GNSS-based
systems. The objective in all cases is to mitigate the effects of the ionosphere
on systems involved (e.g., loss of lock of GNSS receivers) (Bourdillon, France;
Lastovicka, Czech Republic; Cander, U.K.; E. Tulunay, Turkey; Warnant,
Belgium).. COST efforts to establish a good perturbation index have focussed on
squared TEC rates and latitudinal TEC gradients (Jakowski, Germany).
Large-scale theoretical modelling will help to define the indices that are required to accurately include the forcing from below and above in IRI. Examples presented at this meeting are the new Integrated Dynamics through the Earth Atmosphere (IDEA) model of Fuller-Rowell et al. (USA) coupling a Whole Atmosphere Model (WAM) with Global Ionosphere-Plasmasphere (GIP) and electrodynamics models for studying and quantifying terrestrial weather effects, and the Global Self-consistent Model for the Thermosphere-Ionosphere-Plasmasphere (GSM TIP) by Klimenko et al. (Russia) for studying the ionospheric effects of substorms and of a solar eclipse. Using CHAMP, TOPEX, IMAGE, TIMED, COSMIC, and GPS data Watanabe (Japan) and Talaat (USA) presented strong arguments for the need of a strong coupling of IRI with the middle and lower atmosphere.
Statistical studies of the variation patterns of characteristic features in the low and high latitude ionosphere are a first important step towards including these features in IRI. At low latitudes studies are focused on the amplitude and width of the Equatorial Anomaly using GNSS (M.-L. Zhang, China), SROSS C2 (Bhuyan, India), ROCSAT 1 and CHAMP satellite data, at high latitudes the focus is on the sub-auroral trough (Zaalov, U.K.) and modeling is based on GNSS (Krankowski, Poland) and DEMETER data (Rothkaehl, Poland).
As
always a large number of presentations compared the IRI model with local
measurements and models. Al-Ubaidi (Iraq) found good agreement with
measurements by the Al-Battani ionosonde near Baghdad (34.4,44.4) during 1989.
Comparisons with the long record of ionosonde measurements in Hainan, China
showed good agreement for foF2 and discrepancies for hmF2 (X. Wang, China).
Several years of
MF radar (3.17 MHz) measurements of D-region electron densities with the Saura
radar at Andoya island (69¡N) should help to improve the representation of
electron densities from 55 km to 90 km in IRI. The derived electron density profiles
are in general agreement with results from insitu radio wave propagation
experiments at Andenes as well as with observations by the EISCAT VHF radar at
Troms¿ (Latteck, Germany).
MEMBERS, MEETINGS, PUBLICATIONS
Two new members were welcome into the IRI team.
Dr. Wan Weixang from the Institute of Geology and Geophysics in Beijing, China
brings with him his great expertise in
Eigen mode analysis of ionospheric parameters and he will help the IRI
team with access to the Chinese ionosonde data. Dr. K.G. Ratovsky from the
Institute of Solar-Terrestrial Physics in Irkutsk, Russia will take the place
of Dr. E. Kazimirovsky (formerly at the same Institute) who is retiring after
many years of service to the IRI project mostly in the area of ion drift measurements
and modelling.
A
special 2-day IRI session was accepted for the 2008 COSPAR General Assembly in
Montreal, Canada. The session is on the topic of IRI Updating and Data
Assimilation. The next full IRI Workshop will be held near Kagoshima, Japan in 2009. Dr. Watanabe gave a very enticing
presentation about the location for the 2009 IRI Workshop, which will be held
near Kagoshima, Japan, most likely in the fall (October). There are also plans
for a Special Workshop on the Real-time IRI either in Fall of 2008 or Spring
2009 in Boulder, Colorado organized by Tim Fuller-Rowell and Eduardo Araujo.
The
accepted papers from the 2005 IRI workshop in Ebro, Spain were recently
published as Volume 39, Issue 5 of Advances in Space Research with Reinisch,
Bilitza, Altadill as the editors.