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Open
Questions:
[Vasyliunas]
- What is the mechanism
for pre-dipolarization:
Does it start with X-line?
Does it start close in with "instability"?
Does external triggering play a significant frole in substorm
process?
Do instabilities at the inner edge (ballooning, CCI, etc.) lead
to changes of the large-scale magnetic field, and if so, how?
Do the BBF's play any special role in substorms?
[Shiokawa]
- How is growth-phase
stress balance broken - by X-line formation, or by near-Earth
(<10 Re) process?
- Is magnetic flux
to the near-Earth region carried mainly by BBF's or by other
processes?
[Otto]
- What is the source
of E_y to enable dipolarization?
- What makes aurora?
- What is the coupling
between magbetosphere and ionosphere?
[Henderson]
- Is there more
than one "type" of substorm? (i.e. are there different
causes?)
- Must lobe reconnection
occur in every substorm?
- Are all substorms
externally "triggered"?
[Lyons]
- Is the fraction
of substorm onsets that are "caused" by IMF changes
that lead to reduction of convection closer to 50% or to 100%?
[Ridley]
- Does the ionospheric
electric field increase or decrease?
- What is the role
of ionospheric conductance?
- What is the role
of pseudo-breakups in magnetotail "stability" or substorm
development?
[Smith]
- What is the effect
of "unequal" ionospheres (north/south, winter/summer,
B_y modulation) on the substorm processes in the magnetotail?
[Lui]
- Does magnetic
reconnection always produce significant energization of particles
in the magnetotail?
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Personal
statements
(points about which there is no consensus but, in the opinion
of the individual in question, they should be):
[Cheng]
- Complex structures
of auroral breakup correspond to plasma turbulence in the near-Earth
plasma sheet during expansion phase.
- Substorm onset
is initiated by KBI which leads to other instabilities, to form
turbulence and eventually lead to transport of plasma pressure.
- Plasma pressure
transport (reduction) process in near-Earth plasma sheet leads
to dipolarization of B and change of E fields.
[Henderson]
- Magnetic storms
are not equal to summation of substorms.
- Magnetic storms
are not equal to SMC's (steady magnetospheric convection, "convection
bays").
- Auroral substorm
morphology is more complex than the "classical" picture
of Akasofu.
[Lui]
- The substorm expansion
onset process is intimately associated with a strong current
sheet in the near-Earth region.
- Magnetic field
description is equivalent to current description, by Maxwell's
equations.
- There are multiple
activity sites with multiple scales in the magnetotail during
substorm expansion.
- There is a wide
range in the spatial scale and magnitude (energy release) of
magnetotail disturbances, ranging from pseudobreakups to large
substorms covering many local time zones.
[Otto]
- Magnetotail lobe
reconnection occurs in every substorm.
- Current sheet
thinning requires divergent flux transport.
[Shiokawa]
- substorm is the
release of energy stored in the magnetotail as tail-like magnetic
flux (during the growth phase) to the dipolar field region (during
the expansion phase).
- During expansion
phase, significant magnetic flux is carried from NENL and piled-up
in the near-Earth tail.
[Vasyliunas]
- Growth phase produced
by flow that is enhanced in the dayside and reduced in the magnetotail.
- A pre-dipolarization
phase is unavoidable.
- New X-line formed
during every substorm, at what stage (before or after onset)
not yet clear.
[Kan]
- Brightening of
an auroral arc can result from enhanced global convection driven
by enhanced dayside reconnection during the growth phase.
- Dipolarization
in the near-Earth plasma sheet (~6-10 Re) is the cause of the
substorm expansion onset.
- Dipolarization
can result from impeding the enhanced sunward convection on the
earthward side of the dipolarization region in the near-Earth
plasma sheet.
- The cause of impeding
the enhanced sunward convection is not yet understood.
[Swift]
- The major need
are coordinated and adequately financed efforts to develop global-scale
kinetic models of the magnetosheath, magnetosphere, ionosphere
system. Computer technology and algorithms have advanced to the
point where such simulations are feasible. Only few percent of
the support for observations directed into kinetic modeling efforts
will do more resolving the outstanding issues than continued
debate based on more observations.
[Bristow]
- Reconnection in
the tail is necessary to allow tail magnetic flux to replenish
dayside flux removed by subsolar reconnection. This is because
steady convection cannot occur fast enough when dayside reconnection
is rapid and the nightside x-line is in the distant tail. Hence,
while tail reconnection may or may not cause expansion phase
onset, it is a necessary part of a substorm.
- Steady convection
may be possible if the distant tail x-line is near enough to
the earth and the dayside driving rate is low enough so that
tail particle energy can be dissipated in the ionosphere. Under
such conditions, substorms are not necessary for replenishment
of dayside flux.
- The development
of the Harang discontinuity during growth phase and its subsequent
disappearance at expansion onset appear to be a nearly universal
feature of substorms.
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