Title: Observation Of Nuclear Spin Selection Rules In Supersonically Expanding Plasmas Containing H3
1Observation Of Nuclear Spin Selection Rules In
Supersonically Expanding Plasmas Containing H3
Brian Tom, Michael Wiczer, Andrew Mills, Kyle
Crabtree, and Ben McCall
Department of Chemistry
Department of Astronomy
2Motivations
- Source of para-H3
- Dissociative recombination studies
- H3 H2 ? H3 H2
- Simplest reaction of polyatomic
- Interstellar o/p H3
- To/p ? Tkin ??
Cygnus OB2 12
3Para-H2 Para-H2 ? Para-H3 H
n-H2
p-H2
n-H2
p-H2
4Para-H2 Para-H2 ? Para-H3 H
- Produce para-H2
- Ionize para-H2
- React to para-H3
5H3 H2 ? (H5) ? H3 H2
1
identity
H5
3
hop
6
hop/exchange 0.5
exchange
6Dynamics of Reaction
C2v
3000 cm-1
1500 cm-1
50 cm-1
hop
exchange
Not obvious that statistical hop/exchange 0.5
is valid!
7Spin-Modification Probability
Products formed by Hop and Exchange
Reactants
Park Light JCP 126, 044305 (2007)
8Spin-Modification Probability
Products formed by Hop and Exchange
Reactants
1/2 ? 0 ? 3/2 ? 0
1/2 ? 0 ? 3/2 ? 1
Park Light JCP 126, 044305 (2007)
9Low Temperature Effects
- In pure p-H2
- p-H3 ? o-H3 requires p-H2 ? o-H2
ortho I 3/2
para I 1/2
ortho I 1
170 K
para I 0
10Oka Group Experiments
Cordonnier et al. JCP 113, 3181 (2000)
Pulsed Hollow Cathode
Positive Column Cell
reaction not yet measured at low T
p-H3
n-H2
p-H2
p-H2?o-H2
o-H3
p-H3
o-H3
p-H2
n-H2
_at_ 400 K
not 0.5!
11Supersonic Expansion Ion Source
Gas inlet 2 atm
H2
Solenoid valve
- Developed for DR experiments
- H3 formed near nozzle
- p-H2/H2 frozen
- p-H3/H3 evolves, but steady state
- Probed by spectroscopy
McCall et al. PRA 70, 052716 (2004)
122.8 4.8 mm DFG System
NdYAG 1064 nm
532 nm pump laser
l/4
TiSapph 700 990 nm
l/2
AOM
25cm
20cm
reference cavity
Andrew Mills WG10
l/2
PPLN
InSb
mode- matching lenses
ringdown cavity
Glan prism
dichroic
20cm achromat
13Cavity Ringdown Spectra
- First results from our DFG laser!
- Clear enhancement of para-H3 in para-H2
- More enhanced in argon dilution
- Trot 80 K
- R(1,1)u vs R(2,2)l
ortho-H3
para-H3
14Theoretical Predictions
koppo ? k(o-H3 p-H2 ? p-H3 o-H2)
- Steady state
- High temp limit
- Low temp calculations of k by Park Light
Park Light JCP 126, 044305 (2007)
15Comparison with Experiment
Park Light
16H3 toward ? Persei
fp 0.62 0.09
McCall, et al. Nature 422, 500 (2003)
N(H2) from Copernicus
? 0.68 0.20
Savage et al. ApJ 216, 291 (1977)
17Diffuse Clouds Comparison
18Future Directions
- Experiment
- Hollow cathode _at_ 150 K
- Measure H3 and H2
- Expansion source
- Vary ?, T
- Theory
- Different values of a
- Observations
- More sources
- Improved error bars
19Acknowledgments
Brian Tom Michael Wiczer (?MIT) Andrew Mills Kyle
Crabtree Nick Indriolo
NSF Division of AMO Physics
Takeshi Oka (U. Chicago)
Tom Geballe (Gemini)
NASA Laboratory Astrophysics
http//astrochemistry.uiuc.edu