breaking the symmetry in methyl radical: high resolution ir spectroscopy of ch 2 d melanie roberts...
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![Page 1: Breaking the Symmetry in Methyl Radical: High resolution IR spectroscopy of CH 2 D Melanie Roberts Department of Chemistry and Biochemistry, JILA University](https://reader030.vdocuments.us/reader030/viewer/2022032703/56649f535503460f94c779d5/html5/thumbnails/1.jpg)
Breaking the Symmetry in Methyl Radical:
High resolution IR spectroscopy of CH2D
Melanie RobertsDepartment of Chemistry and Biochemistry, JILA
University of Colorado at Boulder National Institute of Standards and Technology
Chandra Savage, Feng Dong, David Nesbitt
![Page 2: Breaking the Symmetry in Methyl Radical: High resolution IR spectroscopy of CH 2 D Melanie Roberts Department of Chemistry and Biochemistry, JILA University](https://reader030.vdocuments.us/reader030/viewer/2022032703/56649f535503460f94c779d5/html5/thumbnails/2.jpg)
Previous Work on CH2D
M. E. Jacox, 1977 Matrix isolation spectroscopy
J. L. Brum et al., 1993 Gas phase, REMPI Electronic structure
K. Kawaguchi, 2001 Gas phase, FTIR Out-of-plane bending mode Q, R branches only
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The Broken Symmetry…
CH3: 1 IR-active stretch doubly-degenerate asymmetric stretch
CH2D: 3 IR-active stretches CH symmetric and CH antisymmetric stretch CD stretch
Hydrogen I=1/2, Deuterium, I=1 CH2D: small dipole moment
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Experimental Setup
•Servoloop locked optical transfer cavities for high frequency precision (~20 MHz)•Servoloop locked optical transfer cavities for high frequency precision (~20 MHz)
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Radical Source
High radical densities at slit (~1014 -1016 /cm3!)
Sub-Doppler molecular linewidths (~40 MHz in Ne expansion)
High radical densities at slit (~1014 -1016 /cm3!)
Sub-Doppler molecular linewidths (~40 MHz in Ne expansion)
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Rotational Energy Levels
220
221
211
212
202
110
111
101
000
Ene
rgy
labels: NKaKc
Watson Hamiltonian
C
B
A
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Nuclear Spin Statistics
Ψ = Ψel Ψvib Ψrot Ψns
- - + + α α
1/√2 (α β +β α)
β β
- - + - 1/√2(α β - β α)
Electronic Vibration Rotation Nuclear Spin
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Experimental Data
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Symmetric Stretch: DFT calculations:
B3LYP/6-311++G(3df,3pd)
Anharmonicity benchmarked to 10 CH radicals
1 10
21
1 1 01
20
21 1
0
21
1 0 00
10
1
1 11
11
0
1 10
11
1
2 11
21
21 0
1
00
0
2 12
11
12 0
2
10
1
2 11
11
0
3 13
21
2
3 03
20
2
3 12
21
1
Predictions
Data
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Boltzmann Plot
Para
Ortho
Trot = 18.9(3) K
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Ground State Rotational Constants
Axis FTIR Studies* (cm-1) This Work (cm-1)
A 9.596969(89) 9.586(8 )
B 5.90686(49) 5.9067(1 )
C 3.6164(10) 3.6195(7 )
*K. Kawaguchi, 2001
Band Origin (cm-1)
3065.64(1)
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What is really happening?
CH bond length increases Ground state: 1.0788(10)Å Excited state: 1.0854(23)Å
Rotational Constant changes (excited state – ground state) ΔA = 0.16 cm-1
ΔB = 0.02 cm-1
ΔC = 0.03 cm-1
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Fine and Hyperfine Terms
ITSH
ITSH
SIaH
SNSNH
eQeQ
DDDD
ff
sr
)(21
Unsplit rotational
level Spin-rotation splitting Nuclear
hyperfine splitting
J = N + S
F1 = J + IH2
F2 = F1 +ID
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Fine and Hyperfine Structure
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Summary CH2D Symmetric Stretch Band
Rotational Structure Fine Structure
Hyperfine Structure
Antisymmetric Stretch
Future Work Oxygenated Radicals
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Acknowledgements•Chandra Savage•Feng Dong•Scott Davis•Erin Whitney•David Nesbitt•OSEP•NSF/IGERT