Title: NIR OFFAXIS ICOS SPECTRUM OF THE NITRATE RADICAL: DOES THE VIBRATIONLESS 2E STATE OF NO3 UNDERGO STA
1NIR OFF-AXIS ICOS SPECTRUM OF THE NITRATE
RADICAL DOES THE VIBRATIONLESS Ã2E? STATE OF NO3
UNDERGO STATIC JAHN-TELLER DISTORTION?
Kana Takematsu and Mitchio Okumura California
Institute of Technology
Pin Chen and Herbert Pickett Jet Propulsion
Laboratory, California Institute of Technology
John F. Stanton University of Texas
WJ10
2Electronic States of NO3
15 089 cm-1
- B 2E? well studied spectrum is broadened by
vibronic interactions
B 2E'
Jahn-Teller active
- Ã2E? only 3 expt. studies to date, vibronic
bands can be rotationally resolved
7 060 cm-1
A 2E?
forbidden
- X 2A2? only recently confirmed D3h geometry
uncertainty in the fundamental assignments
X 2A'2
D3h geometry
What is the nature of the JT effect in NO3? ?
Spectroscopy of the Ã2E? ? X2A2'
3Jahn-Teller Effect in the Ã2E? state
- Eisfeld and Morokuma
- CASSCF, MRCISD, MRCIQ
- JT Stabilization energy 2000 - 3000 cm-1
- Psuedo-rotation barrier 800-1000 cm-1
- Distorted geometry static distortion
- Symmetric geometry dynamic distortion
2B1 minima
4 Full A 2E? ? X 2A2?? Absorption SpectrumDeev,
Sommar, and Okumura, JCP 2005
- Over 50 vibronic bands detected from 6500-11000
cm-1 - Weak bands ? lt 10-20 cm2
- Strong evidence of Jahn-Teller effect
?4 progression 539 cm-1 519
cm-1 547 cm-1
0.2 cm-1 resolution
5The ?4 Asymmetric Bend (e ?) Vibration JT-Active
Mode
Hirota 1998
Rotationally assigned to a D3h symmetric top
6The ?4 Asymmetric Bend (e ?) Vibration JT-Active
Mode
Hirota 1998
Rotationally assigned to a D3h symmetric top
Deev 2005
Contour analysis suggests D3h excited state
geometry in several bands
7The ?4 Asymmetric Bend (e ?) Vibration JT-Active
Mode
Hirota 1998
Rotationally assigned to a D3h symmetric top
Deev 2005
Contour analysis suggests D3h excited state
geometry in several bands
Is the NO3 A state a case of dynamic distortion?
8Herzberg-Teller Selection Rules limit vibronic
levels that are seen
- 41 E? ? e? A1? ? A2? ? E?
9Herzberg-Teller Selection Rules limit vibronic
levels that are seen
ALLOWED
- 41 E? ? e? A1? ? A2? ? E?
FORBIDDEN from ground state v0
level Off-diagonal JT rotational terms More
asymmetry expected
10Herzberg-Teller Selection Rules limit vibronic
levels that are seen
ALLOWED
- 41 E? ? e? A1? ? A2? ? E?
FORBIDDEN from ground state v0
level Off-diagonal JT rotational terms More
asymmetry expected
The more distorted E? levels are dark
11Detection of the v0 level via the hot band
Deev 2005
A 2E?
D3h or C2v?
368cm-1
X 2A'2
D3h
- Contour analysis suggests v0 has asymmetric
geometry - Rotational structure needs to be resolved
12Diode Laser Detection of NO3 A ? X Spectrum
byIntegrated Cavity Output Spectroscopy
- ICOS cw-diode laser, cavity enhanced technique
- Direct absorption method
- New Focus diode laser
- Sensitivity 10-8 /pass
- Resolution 0.002 cm-1
N2O5 ? NO3 NO2 PNO3 1 x 1013 5 x 1014
/cc Ptot 7 Torr
13ICOS Spectrum of the 41 band
0
14Simulations
EOMIP (Stanton)
Symm top
data
15Preliminary Observations on 41 Band
0
- Evidence that symmetry is broken in v0 level
- High density of lines compared to previous v4
spectrum of Hirota et al (1998) assigned to D3h
upper state - Contour analysis inconsistent with D3h geometry
in upper level - Complications
- Lower 41 state (368 cm-1) has not been
rotationally resolved Coriolis coupling, PJT
effects present - Hot band spectra recorded at higher temperatures
have better S/N but are much more congested
16Future Work
- Rotational analysis of the spectrum using SPFIT
- Program is general enough to allow for fitting of
spectra to a Jahn-Teller Hamiltonian of arbitrary
order - Hindered Rotor basis set is more appropriate for
intermediate level of coupling than free rotor or
D3h - Comparison with ab initio EOMIP calculations
- Stanton (UT Austin)
- Adiabatic surface and nonadiabatic couplings
17Thanks
- Prof. Jaron Hansen (BYU)
- Okumura Group
- JPL Spectroscopy Group
- P. Chelin, N. Ibrahim, C. Fellows, J. Orphal
(CNRS-LISA) - NASA UARP
Reminder, check out Stanton Talk Tomorrow
WJ10
18The n2 Umbrella Vibration A JT-Inactive Mode