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November 6, 2010November 6, 2010MWAM 2010
University of IllinoisMWAM 2010
University of Illinois 11
The ortho:para ratio of H3+
in diffuse molecular cloudsThe ortho:para ratio of H3
+ in diffuse molecular clouds
Kyle N. Crabtree, Nick Indriolo, Holger Kreckel, Brian A. Tom, and Benjamin J. McCall
Kyle N. Crabtree, Nick Indriolo, Holger Kreckel, Brian A. Tom, and Benjamin J. McCall
November 6, 2010November 6, 2010MWAM 2010
University of IllinoisMWAM 2010
University of Illinois 22
H3+, Interstellar Chemistry, and
AstrophysicsH3
+, Interstellar Chemistry, and Astrophysics
• Starting point for complex gas-phase chemistry
• Use as an astrophysical probe:
– Gas density at the galactic center
– Imaging of Jupiter’s polar aurorae
– Interstellar cosmic ray ionization rate
– Interstellar temperature
• Starting point for complex gas-phase chemistry
• Use as an astrophysical probe:
– Gas density at the galactic center
– Imaging of Jupiter’s polar aurorae
– Interstellar cosmic ray ionization rate
– Interstellar temperature
November 6, 2010November 6, 2010MWAM 2010
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University of Illinois 33
H3+ SpectroscopyH3+ Spectroscopy
R(1,0)36685 Å
R(1,1)u
36681 Å
R(1,1)l
37155 Å
November 6, 2010November 6, 2010MWAM 2010
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H3+ as an Interstellar
ThermometerH3
+ as an Interstellar Thermometer• Observed R(1,0)
and R(1,1)u/R(1,1)l lines n(1,0), n(1,1) T(H3
+)
• Analogous to T01, derived from UV observations of H2 J=0 (para) and J=1 (ortho) levels
• Observed R(1,0) and R(1,1)u/R(1,1)l lines n(1,0), n(1,1) T(H3
+)
• Analogous to T01, derived from UV observations of H2 J=0 (para) and J=1 (ortho) levels
November 6, 2010November 6, 2010MWAM 2010
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Temperature in Diffuse Molecular CloudsTemperature in Diffuse Molecular Clouds• Diffuse molecular clouds: diffuse clouds
with most hydrogen in molecular form.• Survey of diffuse molecular clouds:
– <T01> ~ 70 K (N = 66) 1
– <T(H3+)> ~ 30 K (N = 18) 2
• Only 2 are in common: ζ-Per and X-Per• Recent observations (N. Indriolo) have
extended this number to 5
• Diffuse molecular clouds: diffuse clouds with most hydrogen in molecular form.
• Survey of diffuse molecular clouds:– <T01> ~ 70 K (N = 66) 1
– <T(H3+)> ~ 30 K (N = 18) 2
• Only 2 are in common: ζ-Per and X-Per• Recent observations (N. Indriolo) have
extended this number to 51 1 B. D. Savage B. D. Savage et al.et al., , ApJApJ, (1977), , (1977), 216216, 291, B. L. Rachford , 291, B. L. Rachford et al.et al., , ApJApJ, (2002), , (2002), 577577, 221, B. L. , 221, B. L. Rachford Rachford et al.et al., , ApJSApJS, (2009), , (2009), 180180, 125., 125.22 N. Indriolo N. Indriolo et al.et al., , ApJApJ, (2007), , (2007), 671671, 1736., 1736.
1 1 B. D. Savage B. D. Savage et al.et al., , ApJApJ, (1977), , (1977), 216216, 291, B. L. Rachford , 291, B. L. Rachford et al.et al., , ApJApJ, (2002), , (2002), 577577, 221, B. L. , 221, B. L. Rachford Rachford et al.et al., , ApJSApJS, (2009), , (2009), 180180, 125., 125.22 N. Indriolo N. Indriolo et al.et al., , ApJApJ, (2007), , (2007), 671671, 1736., 1736.
November 6, 2010November 6, 2010MWAM 2010
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Temperature DiscrepancyTemperature Discrepancy
ζζ-Per-Per
X-PerX-Per
HD 73882HD 73882
HD 154368HD 154368
HD 110432HD 110432
T(HT(H33++))
TT0101
Which of these Which of these represents the represents the “true” kinetic “true” kinetic temperature?temperature?TT0101
Why is there more Why is there more pp-H-H33
++ than than expected for the expected for the
temperature?temperature?
November 6, 2010November 6, 2010MWAM 2010
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Chemistry of H3+Chemistry of H3+
• Formation:1. H2 + cosmic ray H2
+ + e- (slow)
2. H2+ + H2 H3
+ + H (fast)
• ThermalizationH3
+ + H2 H2 + H3+
• Destruction:H3
+ + e- H2 + H or 3H
• Nuclear spin dependence?
• Formation:1. H2 + cosmic ray H2
+ + e- (slow)
2. H2+ + H2 H3
+ + H (fast)
• ThermalizationH3
+ + H2 H2 + H3+
• Destruction:H3
+ + e- H2 + H or 3H
• Nuclear spin dependence?
November 6, 2010November 6, 2010MWAM 2010
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H3+ FormationH3+ Formation
1. H2 + cosmic ray H2+ + e- (slow)
2. H2+ + H2 H3
+ + H (fast)
1. H2 + cosmic ray H2+ + e- (slow)
2. H2+ + H2 H3
+ + H (fast)
ReactionCollision Fraction
Branching Fraction p-H3
+ p-H3+ Fraction
p-H2+ + p-H2
(p2)2 1 (p2)2
p-H2+ + o-H2
(p2) (1-p2) 2/3(2/3) (p2) (1-
p2)
o-H2+ + p-H2
(1-p2) (p2) 2/3(2/3) (1-p2)
(p2)
o-H2+ + o-H2
(1-p2)2 1/3 (1/3)(1-p2)2
Total(1/3) + (2/3)p2
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“Nascent” p-H3+ Fraction (p3)“Nascent” p-H3+ Fraction (p3)
November 6, 2010November 6, 2010MWAM 2010
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Thermalization: H3+ + H2Thermalization: H3+ + H2
“identity”“identity”
“hop”“hop”
“exchange”“exchange”
H5+H5+
11
33
66
• Branching fractions: Sid, Shop, and Sexch
• α ≡ Shop/Sexch (0.5?)• Selection Rules
• Branching fractions: Sid, Shop, and Sexch
• α ≡ Shop/Sexch (0.5?)• Selection Rules
Does the steady state of this reaction give a thermal ortho:para H3
+ ratio at low temperature?
Does the steady state of this reaction give a thermal ortho:para H3
+ ratio at low temperature?
November 6, 2010November 6, 2010MWAM 2010
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University of Illinois 1111
Bimolecular Reactive Equilibrium (BRE)Bimolecular Reactive Equilibrium (BRE)• n(H2)/n(e-) ~ 104; k(H2,H3
+)/kDR ~ 10-9/10-7 ~ 10-2
• H3+ sees ~100 collisions with H2 during its
lifetime
• Assume steady state [p-H3+] is determined
by nuclear-spin-changing collisions with H2:
• Express in terms of p-H3+ fraction (p3):
• n(H2)/n(e-) ~ 104; k(H2,H3+)/kDR ~ 10-9/10-7 ~
10-2
• H3+ sees ~100 collisions with H2 during its
lifetime
• Assume steady state [p-H3+] is determined
by nuclear-spin-changing collisions with H2:
• Express in terms of p-H3+ fraction (p3):
o-H3+ + p-H2 p-H3
+ + o-H2o-H3+ + p-H2 p-H3
+ + o-H2
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Nuclear Spin Rate CoefficientsNuclear Spin Rate Coefficients
Parameter
Value(s)
Trot 10 K
Tcoll 10-160 K
Sid 0.1-0.9
Shop 0-1
Sexch 0-1
koooo kooop koopo koopp
kopoo kopop koppo koppp
kpooo kpoop kpopo kpopp
kppoo kppop kpppo kpppp
f (T,Sid,)
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p3 vs. p2 Determinationp3 vs. p2 Determination
Trot = 10 KChoose Sid,
α
November 6, 2010November 6, 2010MWAM 2010
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p3 vs. p2 Determinationp3 vs. p2 Determination
Tcoll p2
November 6, 2010November 6, 2010MWAM 2010
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BRE ResultsBRE Results
Sid = 0.9
Sid = 0.1
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BRE ResultsBRE Results
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Steady State ModelSteady State Model
• Include nuclear spin dependent formation and destruction reactions:
• Include nuclear spin dependent formation and destruction reactions:
ke,o = o-H3+ DRke,o = o-H3+ DR
ke,p = p-H3+ DRke,p = p-H3+ DR
xe = Electron fraction (1.5 x 10-4)
f = Molecular fraction (0.9)
xe = Electron fraction (1.5 x 10-4)
f = Molecular fraction (0.9)
November 6, 2010November 6, 2010MWAM 2010
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Steady State: DR Rates EqualSteady State: DR Rates Equal
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Steady State: DR Rates EqualSteady State: DR Rates Equal
November 6, 2010November 6, 2010MWAM 2010
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Steady State: Theoretical1 DR RatesSteady State: Theoretical1 DR Rates
p-H3+ DR 10x faster
than o-H3+
1dos Santos et al., J. Chem. Phys. (2007), 127, 124309.1dos Santos et al., J. Chem. Phys. (2007), 127, 124309.
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Steady State: DR OnlySteady State: DR Only
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ConclusionsConclusions• H3
+ ortho:para ratio in diffuse molecular clouds likely governed by competition between thermalization (H3
+-H2 collisions) and destruction by DR with electrons
• H3+ + H2 reaction based on
microcanonical statistical model– quantum scattering calculations and experimental measurements needed
• State-selective DR measurements of H3+
also needed to verify/invalidate model
• H3+ ortho:para ratio in diffuse molecular
clouds likely governed by competition between thermalization (H3
+-H2 collisions) and destruction by DR with electrons
• H3+ + H2 reaction based on
microcanonical statistical model– quantum scattering calculations and experimental measurements needed
• State-selective DR measurements of H3+
also needed to verify/invalidate model
November 6, 2010November 6, 2010MWAM 2010
University of IllinoisMWAM 2010
University of Illinois 2323
AcknowledgementsAcknowledgements
• McCall group• Takeshi Oka• Steve Federman• Brian Rachford
• McCall group• Takeshi Oka• Steve Federman• Brian Rachford