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Is HO 2 + a Detectable Interstellar Molecule?. Susanna L. Widicus Weaver Departments of Chemistry and Astronomy, University of Illinois at Urbana-Champaign Current address: Department of Chemistry, Emory University David E. Woon - PowerPoint PPT Presentation
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Is HO2+ a Detectable Interstellar Molecule?
Susanna L. Widicus WeaverDepartments of Chemistry and Astronomy, University of Illinois at Urbana-Champaign
Current address: Department of Chemistry, Emory University
David E. WoonDepartment of Chemistry, University of Illinois at Urbana-Champaign
Branko RuscicChemical Sciences and Engineering Division, Argonne National Laboratory
Benjamin J. McCallDepartments of Chemistry and Astronomy, University of Illinois at Urbana-Champaign
Larsson et al., 2007, A&A 466, 999
Interstellar O2
X(O2)
Predicted: 5-10 × 10-6
Odin, -Oph: 5 × 10-8
SWAS limits: < 3 × 10-7
O2 Detection Difficulties
O2
• No permanent electric dipole moment
• Weak magnetic dipole-allowed transitions
• Atmospheric spectral interference
An O2 tracer? HO2+
• a = 1.518 Db = 1.934 D
• Strong millimeter and submillimeter spectrum
• Can be observed from ground-based observatories
Is HO2+ observable?
Interstellar HO2+ Chemistry
H3+ + O2 HO2
+ + H2
Formation:
Destruction: Reverse of this same reaction.
)H(
)O()H()HO(
2
23
1
12
n
nn
k
kn
When steady-state is reached, a true
chemical equilibrium exists!
)H(
)O()H(
2
23n
nnKT
)HO( 2n
kT
E
)O()H(
)H()HO(570.0
23
220
intint
intintT
qqeK
Required Information?
)H(
)O()H(
2
23n
nnKT
)HO( 2n
TkT
E
T QeK0
1.
)O()H(
)H()HO(
23
22
qqQT
2.
)X(2
)X()X()X(2
3
2 intinttr qVh
mkTqqq
3.
)O()H(
)H()HO(570.0
23
22
intint
intint
)O()H(
)H()HO(
)O()H(
)H()HO(
23
222
3
23
22
intint
intint
Tqq
mm
mmQ
4.
where E0/k = rH°/R
Experimental HO2+
Thermochemistry Results
rH°298
(kJ/mol)rG°298
(kJ/mol)Reference
-0.16 ± 0.57 -0.16 ± 0.57 Fennelly et al. (1973)
-1.5 ± 1.4 Fehsenfeld et al. (1975)
-2.1 ± 1.9 Fehsenfeld et al. (1975)
-2.0 ± 1.0 -1.7 ± 1.0 Kim et al. (1975)
-0.0 ± 0.15 -3.0 ± 1.5 Hiraoka et al. (1979)
1.4 ± 3.3 -1.7 ± 1.5 Bohme et la. (1980)
1.4 ± 0.3 -1.48 ± 0.49 Adams & Smith (1984)
1.3 ± 11 -1.6 ± 11 Hunter & Lias (2005)
Ruscic et al. suggest rH°298 = - 0.2092 kJ/molRuscic et al., J Phys Chem A (2006) 110, 6592
Active Thermochemical Tables
Traditional compilations – sequential approach
• available information used only partially• propensity to develop cumulative errors• assigned uncertainties do not properly reflect the available knowledge• contain a hidden maze of progenitor-progeny dependencies
ATcT approach – simultaneous analysis of interdependencies
• solutions reflect cumulative knowledge of network• propagates new knowledge by solving entire network from scratch• points to new experiments by isolating “weak links”• complete covariance matrix available: prevents inflation of uncertainties
ATcT Results for HO2+
rH°298 = 1.31 ± 0.11 kJ/mol
rG°298 = -1.75 ± 0.11 kJ/mol
Partition Functions
Equilibrium Constant
Nuclear Spin Selection Rules
O2 +
22.8 cm-1
0 cm-1
o-H3+
p-H3+
o-H2
p-H2
0 cm-1
118.5 cm-1
+ HO2+
2/3
1/2
1/21/3
1
1
O2 + p-H3+ → p-H2 + HO2
+ k = k1/4so K = KT/4
Spectral Prediction
T = 100 K
Simulated with PGopher (Western 2007) using constants from previous talk.
Is Interstellar HO2+ Detectable?
• Transitions? - B, C are known to ~40 MHz- A is known to ~5 GHz
• Temperature?- intensities scale as (KT/QT)e-Eu/kT
• Sources?- high n(H3
+) - T~100 K
1 0 1 0 0 0
at 47.2, 102.5, 412.9 GHz
100 K
hot cores
Is Interstellar HO2+ Detectable?
)H(
)O()H(
2
23n
nnKT
)HO( 2n
(10-4 cm-3) (10-5)0.6765
7×10-10 cm-3
For L = 1 pc, NT = 2×10-9 cm-2
TMB ~ 6×10-5 K!!
Clearly, HO2+ is not detectable
ConclusionsMost accurate theoretical investigation of HO2
+ to date:
• Thermochemistry- HO2
+ formation rH°298 = 1.31 ± 0.11 kJ/mol
• Molecular constants, dipole moment - Rotational spectral prediction
• Examination of interstellar chemistry, likelihood of detection
- Unusual case of interstellar chemical equilibrium
- Line intensities ~ 60 K- HO2
+ not detectable
Acknowledgements• NSF CAREER award (NSF CHE-0449592) • UIUC Critical Research Initiative program• Prof. Thom H. Dunning, Jr.• Office of Basic Energy Sciences, Division of Chemical Sciences, Geosciences, and Biosciences, US Department of Energy, contract number DEAC02-06CH11357• Task Group of the International Union of Pure and Applied Chemistry (IUPAC) on `Selected Free Radicals and Critical Intermediates: Thermodynamic Properties from Theory and Experiment' [IUPAC Project 2003-024-1-100