Title: SHINE 2006
1Review of CIR-related Particle Composition,
Charge States, Energy Spectra
Joe Mazur The Aerospace Corporation Glenn
Mason Johns Hopkins/APL Joe Dwyer Florida
Institute of Technology Mihir Desai Southwest
Research Institute
2Processes for 1 AU observations of solar material
After Stone et al., Space Sci Rev., 86, 1, 2000
35 AU
1 AU
Desai et al., JGR, 104, 6705, 1999
Mason et al., ApJ Letters, 486, L149, 1997
4Stream interface
5Abundances
Mason et al., ApJ Letters, 486, L149, 1997 see
also Richardson et al., JGR 98, 13, 1993
6Ratios vs. solar wind speed
7Abundance summary
- similar to solar system except for factor of 2-3
enhancement of He and C/O - increase of He/O, C/O, and Ne/O with solar wind
speed - He abundance increases from 1 to 5 AU
Mason von Steiger et al. Space Sci. Rev. 89,
1999 (ISSI CIR Workshop held in 1998)
8Ulysses 4.5 AU
Pick up ion He increases its contribution to
CIRs at greater radial distances Suggested that
other pickup ions (such as inner source) at 1 AU
might account for some puzzling composition
observations
Gloeckler et al., JGR, 99, 17637, 1994.
9Acceleration of suprathermal He in CIRs
enhanced 103 - 104 over solar wind
Chotoo et al., JGR, 105, 23107, 2000.
10Mazur et al. ApJ 566, 2002
Mobius et al. Geophysical Research Letters, 29,
2001
11Averaged CIR charge states 0.5 MeV/n
Species SAMPEX ACE
He 2.000.12 -
C 4.830.27 5.10.3
O 6.120.37 6.10.35
Ne 7.250.25 7.80.5
Fe 13.000.48 10.50.6
Mobius et al. Geophysical Research Letters, 29,
2001
Mazur et al. ApJ 566, 2002
12Möbius et al., AIP Conf. Proc. 598, 201, 2001
13Charge state summary
- More pickup He at 4.5 AU than 1 AI (at 1 AU the
pickup He is 15 He, while at 4.5 AU it is
twice as abundant) - Heavy ions at 1 AU show little evidence of pickup
species
14Mason et al., ApJ Letters, 486, L149, 1997
15Summary
- Abundances
- Ion composition similar to solar system but with
some differences - Still puzzling dependence of some ratios on
solar wind speed - Charge states
- Little evidence of Zgt2 pickup ions at 1 AU
- Large abundance of pickup helium at 5 AU
- Energy spectra
- Power law from tens of keV/n to 1 MeV/n
- Steepening above 1 MeV/n
- Spectral forms do not change out to 10s of AU
- The source population is coming from the
suprathermal region, but that population is not
just heated solar wind other constituents are
important - Most often the 1 AU particles are not accelerated
at shocks requiring another mechanism (Jokipii et
al. 2003) - As we approach solar minimum we have the
opportunity to revisit some of these observables
with ACE
16Essential new work needed
- Complete ACE surveys with much larger number of
species identified - fully characterize properties of suprathermal /
pick-up ion distributions - detailed theoretical models to probe injection
issues
17C. Chotoo, Ph.D. thesis, U of Maryland 1998
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20Energy spectra summary
- power law from tens of keV/n to 1 MeV/n
- steepening above 1 MeV/n
- spectral forms do not change out to 10s of AU
See also Mason von Steiger et al. Space Sci.
Rev. 89, 1999 (ISSI CIR Workshop held in 1998)
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22Energy spectra summary
- More pickup He at 4.5 AU than 1 AI (at 1 AU the
pickup He is 15 He, while at 4.5 AU it is
twice as abundant) - Heavy ions at 1 AU show little evidence of pickup
species
23Möbius et al., AIP Conf. Proc. 598, 201, 2001
24Möbius et al., AIP Conf. Proc. 598, 201, 2001
25Richardson et al., JGR, 98, 13, 1993
26Dwyer et al, in preparation, 2002
27Fisk Lee acceleration model--
- particles in CIRs accelerated by compression at
forward and reverse shocks at several AU
propagate in to 1 AU - adiabatic deceleration in solar wind included
- yields distribution function spectra and
gradients similar to observations above 100
keV/n - injection energy gt 5 keV required, ie from
postulated suprathermal tail of the solar wind - composition similar to source material (assumed
to be solar wind suprathermal tail) -- (note no
systematic measurements of solar wind comp.
available at that time)
L. A. Fisk and M. A. Lee, Astrophys. J., 237,
620, 1980
28Suprathermals as a seed population--
- SEP related events
- super events in the inner solar-system (Dröge
et al. 1992.) - Peak intensities in August 1972 (Smart et al.
1990) - Interplanetary shocks
- Aug 1978 shock (Gosling et al. 1981)
- IP shock survey (Tsurutani Lin 1985)
- Sources?
- long lived remnants of solar flares
- planetary bow shocks
- corotating interaction regions
29Fisk Lee CIR spectral form--
CIR spectral form where v particle speed
r radius of observer rs shock radius ??
shock strength ???diffusion coefficient? V
solar wind speed
30CIR model status 1970s-80s
- Successful
- spectra above 100 keV/n
- composition similar to (unmeasured) solar wind
- origin at several AU, and gradients
- Not successful / unaddressed
- C/O ratio
- spectral forms vs. compression ratios
- intensities
31New CIR energetic particle observations
challenges to standard model--
- Particle spectra continue to rise down to 10
keV/nucleon at 1 AU - C/O ratio dependence on solar wind speed
- Mg/O shows no FIP effect
- large abundance of He at 1 and several AU
- 3He abundance enhanced compared to solar wind
32Butter Garlic Croutons Enriched unbleached
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solids, yeast, salt, contains 2 or less of the
following whey, maltodextrin, wheat gluten,
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TBHQ (to preserve freshness).
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34Hilchenbach et al., Trnas. Am.Geophys. U., 78,
F554, 1997
35Interstellar Gas Flow in Inner Solar System
From University of New Hampshire group WWW
page http//www-ssg.sr.unh.edu/tof/Missions/Ace/ac
eset.html
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373He is enriched in CIRs -- about 4 times the
solar wind value compared to 4He
Dwyer et al, in preparation, 2002
38Role of pick up ions --
- consistent with He abundance
- tempting explanation for C/O ratio, but
- no seasonal variation of heavy ion abundances
detected, but data is sparse - at 1 AU C is a small fraction of CIR carbon
39CY 1994, ltrgt 2.8AU ltlatitudegt -65 ltvswgt784
km/s
Gloeckler Geiss, Space Sci. Rev, 86, 127, 1998
40SAMPEX geomagnetic latitude cutoffs of (a) 14
CIRs (1992- 95), and (b) all 1998 SEP events
Mazur, Mason Mewaldt, 2002, ApJ, in press
41SAMPEX Calibration of adjusted magnetic
invariant latitude cutoffs for CIRs and SEP
events
Mazur, Mason Mewaldt, 2002, ApJ, in press
42 SAMPEX Observed magnetic cutoffs for CIR
events, vs inferred cutoff if ions were singly
ionized. Singly stripped ions must be no more
than a few percent of total.
Mazur, Mason Mewaldt, 2002, ApJ, in press
43CIR abundance details show that bulk solar wind
source does not fit the new observations--
- Source population is coming from suprathermal
region, but that population is not just heated
solar wind -- other constituents important - Do other shock-associated energetic particle
observations show evidence for suprathermal seed
ions? YES SEPs, ESPs -- tracer ion is 3He
443He and 4He time intensity profiles in large
June 4, 1999 solar particle event
Mason et al., Ap.J. Letters, 525, L133, 1999
45Enhanceed abundances of 3He in large SEP events
ACE/SIS 8-13 MeV/n
ACE/ULEIS 0.5-2 MeV/n
Wiedenbeck et al., AIP Conf Proc 528, 107, 2000
Mason et al., Ap.J. Letters, 525, L133, 1999
46Suprathermals show 10-100 times more variation in
intensity than solar wind -- likely critical
issue in energetic particle intensities
47Conclusions 1 AU CIRs
- CIR source is not bulk solar wind, but rather the
suprathermal region (v/vsw gt 1.5) - time dependent, multiple ingredients
- solar wind suprathermal tail
- pick up ions (interstellar)
- pick up ions (inner source)
- other remnants (large SEP events, impulsive SEP
events) - at lt few hundred keV/n, CIR ions are locally
accelerated
48- CIRs observed in early 2000 on ACE
- typical appearance
- note change in C/O ratio in CIRs vs. solar events
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51Introduction
- Dependence of some abundances on coronal hole
speed - No reflection of solar wind abundance changes
across stream interface - pointing to another
source (the suprathermals) / Ubiquitous tails - Little influence of Zgt2 pickup ions at 1 AU
- Most 1 AU events dont have shocks
- complicated time profile that includes local
acceleration and transport of ions from shocks
later in the events, as long as a week (Reames)