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Description of the Electron Spin-Angle Distribution Plots
John Steinberg Mar 6, 2002
General
In each panel, the relative electron flux at
a given energy is represented using a color scale, the highest flux being red.
The electron flux is plotted as a function of spacecraft spin angle (vertical
axis) and time (horizontal axis). Genesis is oriented with the spin axis vector
lying in the ecliptic and generally pointed sunward. The spin angle (vertical
axis) value of 0° , or equivalently 360° , corresponds to the position where
the GEM aperture look direction is northward. Strictly speaking, it is not the
electron flux that is plotted, but rather a reduced distribution function
value. But you need not understand what is meant by "reduced distribution
function" in order to use these plots to make qualitative conclusions
about the solar wind electrons. The dedicated reader will find the reduced
distribution function explained at the bottom of this page.
Coronal hole and interstream solar wind
Measured in the vicinity of Earth, solar wind electrons at energies above about 100
eV can generally be considered to be supra-thermal electrons.
The supra-thermal electrons
typically do not have the same
flux in all directions. Rather, these electrons usually have a flux peaked
along a direction parallel (or anti-parallel) to the local interplanetary
magnetic field direction. As the Genesis spacecraft rotates, the field of view
for GEM sweeps across the interplanetary magnetic field direction. GEM then
detects a peak flux centered at the spin angle into which the field direction
projects. For ordinary stationary solar wind flows ( i.e. not coronal mass
ejection transient ) the supra-thermal electrons stream away from the sun along
magnetic field lines having only one foot in the solar corona. The electron
flux is uni-directional, and GEM detects a peak flux only once per spin.
Here is an example of a well-defined uni-directional electron flux
from the Genesis Browse plots

The time interval shown is 1 day.
The single red "stripe"
is the uni-directional
supra-thermal electron flux. Note that the peak angle is not steady, but has
some jitter. This is because the interplanetary magnetic field, which is
guiding the electrons, is not steady but fluctuates.
Coronal mass ejection solar
wind
At times, the supra-thermal electrons exhibit
peak flux both parallel and anti-parallel to the interplanetary magnetic field.
This phenomenon is often refered to as "counter-streaming electrons"
or "bi-directional electron streaming" (BDES). The interplanetary
magnetic field within many coronal mass ejection (CME) transient flows
is believed to
form loops that return to the solar corona along both directions. Observation
of BDES is interpreted to be a probable indicator of those closed loops.
However, BDES does not occur exclusively within CMEs, but can occur for other
reasons as well.
Thus, the Genesis regime selection algorithm does not select the CME regime
based on BDES alone. An additional CME indicator is required.
When
the electron flux is bi-directional, GEM will detect a peak flux twice per
spin, and the two peaks will be 180° apart.
Here are several one-day examples of good coronal mass ejection-related
bi-directional electron streaming:

Above is a "typical best example" day.

Early on this day, passage of an
interplanetary shock is seen by the high flux filling in at all angles.
Post-shock, we see two distinct beams emerge. Note that the plot
"wraps" in angle: the peak flux at 0° and at 360° are from the same
beam!

Above is a one-day example exhibiting a distinct onset of BDEs.
Solar energetic particle events
One a few occasions, GEM has been hampered by
the effects of solar energetic particle events. The penetrating particle
radiation results in a high background count rate for GEM which overwhelms the
solar wind electron count rate. This is an infrequent occurrence. However, you
may notice the plots going "all red" when SEP events happen.
(Please not that "all red" does not necessarily mean
the instrument saturated; it may simply be that the color scale for
plotting reached saturation, but not the instrument.)
Here is what the one-day plots look like when
solar energetic particles
produce a high background count rate:

And the kitchen sink
Above we have shown examples of clear
uni-directional electrons, and clear bi-directional electrons. But, as you may
have guessed, the signatures in the browse data plots are not always so clear
or persistent. The example below shows a variety of features all on one day.
The electron signiture is initially indeterminate, follow by intervals which
are uni-directional, and intermittantly bi-directional. Finally at the end of
the day the signatures are indeterminate again. We also show the bottom panel
from the Genesis Browse Solar Wind summary plot for the same time interval.
Compare for yourself the results obtained from the autonomous onboard BDE
detection algorithm to the Electron Spin-Angle Distribution plot.
Here is a day of Genesis observations with some uni-directional
electrons, some bi-directional electrons, and some intervals which are
indeterminate.


As you use the Browse data plots, you will
probably find it useful to swtich back and forth between the Solar Wind summary
plot and the Electron Spin Angle Distribution plot, and compare the autonomous
BDE detection algorithm results to the color plots.
What
we really plot: the reduced distribution function
From the counts accumulated by the Genesis
Electron Monitor, we obtain the electron distribution function
![]()
which has units of
( electrons) /
( (cm-3)(cm/s)-3)
The variables
,
and
are defined as
follows:
Particle speed (cm/s)
Polar
angle relative to the spacecraft spin axis vector direction
Azimuth angle or spacecraft spin angle
The distribution function is defined so that
the electron number density n (cm-3) is obtained
when the distribution function is integrated over all velocity space as
follows:
![]()
The
quanitity whose magnitude is represented by color intensity in the Genesis
"spin angle plots" is the distribution function where we have
integrated over the polar angle.
![]()
which still has units of
( electrons) /
( (cm-3)(cm/s)-3)
How
to use the color scale bar

The scale bar on the right hand side of each
plot indicates the range of values of distribution function covered by the
color bar within each plot. The color scale is DIFFERENT FOR EACH PANEL!
The color red does not indicate the same flux in different panels.
The table below indicates how to interpret the
color scale within each panel of the plot fragment shown above.
The thick line segments by each panel indicate how the range displayed
for a given panel compares to the total sensitivity range of GEM.
|
Range of distribution function value for each panel |
||
|
PANEL |
BLUE minimum value of (cm-3)(cm/s)-3 |
RED maximum value of (cm-3)(cm/s)-3 |
|
TOP |
1.7x10-32 |
32 x10-32 |
|
5 |
5.6 x10-32 |
120 x10-32 |
|
4 |
1.9 x10-31 |
46 x10-31 |
|
3 |
6.3 x10-31 |
172 x10-31 |
|
2 |
2.1 x10-30 |
66 x10-30 |
|
Bottom |
7.3 x10-30 |
251 x10-30 |
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