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			 **   THE GEM MESSENGER   **
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						     Volume 10, Number 38
						     September 12, 2000
						     
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1. Your Input Required for JGR Special Section on Substorm Onset Timing 
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From: Shin Ohtani <ohtani at fluxgate.jhuapl.edu>

Substorm onset timing has been the main target of the GEM T/S observation
working group (see the group report of this issue of the GEM messenger).  We
are currently considering a special section for JGR on this subject.
According to Janet Luhmann, the senior editor of JGR, the review process of
papers submitted to a special section is the same as that of regular papers,
but they will be published under a special section title to gain higher
publicity.  Although the T/S observation working group has been focusing on
satellite and ground measurements, the special section, if realized, will be
open to all approaches including theory and model calculations.
Contributions from outside of the group of regular attendees of the GEM
workshop will also be welcome.  It is, however, uncertain at present whether
there exists sufficient interest for proposing this idea to the JGR
editorial office.  We would be most grateful if you could inform us of your
interest at ohtani at jhuapl.edu. 

Mark Moldwin and Shin Ohtani (Co-chairs)

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2. GEM Tail/Substorm Observation Working Group Report of the 2000 Snowmass
   Workshop
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From: Shin Ohtani <ohtani at fluxgate.jhuapl.edu>

The T/S observation workshop group had two sessions in Snowmass this year.
In one session the working group discussed substorm onset timing focusing on
the timing of the Pi2 onset relative to the auroral breakup.  The other
session was devoted to other substorm-related phenomena with an emphasis on
near-Earth substorm processes.

I. SUBSTORM ONSET TIMING

Substorm onset timing has been the main subject of this working group.
Whereas the Pi2 onset is often used as a substorm identifier, its timing
relative to the auroral breakup has not been tested statistically until
recently.  Liou et al. [JGR, 105, p.2495, 2000; also presented at previous
GEM workshops] reported that Pi2 onsets observed at a low-latitude ground
station tend to be delayed from auroral breakups identified from Polar UVI
images.  In the session Kawano/Uozumi reported their model calculation of
Pi2 propagation in the near-Earth tail.  The propagation speed is
significantly slower in the plasmasphere because of the high plasma density
there, which affects the Pi2 onset time at low latitudes but not at high
latitudes, providing an explanation for the delay of the low-latitude Pi2
onset.  Lu reported an event observed by ground stations distributed
globally, which indeed reveals a complicated spatial distribution of the
onset time.  Kepko proposed to use several stations at mid/low latitudes in
the substorm onset sector for determining the onset time of Pi2.  Whereas
the onset determined in such a way presumably provides the earliest Pi2
onset, it is a separate issue whether or not that onset is coincident with
the corresponding auroral breakup.  Readers who are more interested in this
issue are referred to Kepko and McPherron's comments on Liou et al. [2000]
and the reply to the comments, which will appear in JGR in the near future.
Kepko and Ohtani/Liou pointed out that it requires caution to using the FFT
to determine the Pi2 onset.  The Pi2 wave is often superposed to the
positive bay.  In such a case filtered data could identify a start time
earlier than the actual onset.  Whether it is filtered or not, the
determination of the Pi2 onset is very often based on the visual inspection
of data plots.  It is a consensus of the working group that we need a
quantitative criterion; an example was presented by Kepko.  Whereas the
delay of the Pi2 onset tends to be emphasized, another issue about the Pi2
wave is that according to Liou et al. [2000], very often Pi2 onsets cannot
be associated with any clear auroral breakup, as pointed out by Ohtani/Liou.
It is therefore suggested to avoid counting only on the Pi2 wave for
identifying the substorm onset and to cross-examine other substorm
identifiers, preferably auroral images.

II. NEAR-EARTH SUBSTORM PROCESSES

In the second session presentations were made about various subjects.
Following are brief summaries:

> Lyons suggested from the timing of the Geotail observation of plasma-sheet
convection flows that a NENL is formed after a substorm onset.

> Lu mapped FAC distributions deduced from ground magnetometer data to the
equatorial region and suggested that the maximum FAC originates from the
near-Earth (< 10 RE) region.  The result also indicates the tailward
expansion of the auroral source region.

> Li reported geosynchronous injection events observed at storm time.
Particle tracing he carried out suggests that in one particular event
particles are accelerated on the dayside, rather than nightside, by a
magnetospheric compression.

> Nose' examined the enhancement of energetic O+ fluxes in the plasma sheet
at substorm.  He suggested that O+ ions are accelerated locally by inductive
electric field associated with dipolarization.

> Lessard reported auroral observations by CANOPUS & FAST during the growth
phase and discussed data in terms of the M-I coupling.

> Toivanen showed substorm signatures observed by the Polar satellite in the
polar region and discussed the tail substorm dynamics by mapping them to the
equatorial region.

> Russell pointed out two types of auroral substorms, one triggered near the
poleward edge of the oval and the other at the equatorward edge.  He
interpreted them in terms of distant and near-Earth neutral lines.

> Ohtani reported a current disruption event observed by AMPTE/CCE and
suggested from the anisotropy of energetic ion fluxes that the tail current
is intensified explosively just prior to local dipolarization.

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