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Lineshape Analysis of Dynamic Rotational Spectra in the Presence of Internal Angular Momentum
Brooks H. Pate, Gordon G. Brown, and Justin L. Neill Department of Chemistry University of Virginia
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Dynamic Rotational Spectroscopy
Rotational Spectroscopy of Highly Vibrationally Excited Molecules Intramolecular Vibrational Energy Redistribution (IVR) Causes Time-Dependent Molecular Structure These dynamics lead to frequency modulation effects known in NMR spectroscopy (Dynamic NMR: motional narrowing and coalescence)
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New Effects Unique to Rotational Motion: Gyroscope Dynamics from Internal Angular Momentum
Methylbutenyne V3 = 700 cm-1
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Rotational Transitions MBEY Transition Intensities MBEY
A Sym. E Sym. Kr = 0 (Gyro.) Kr = 0 (Gyro.) Ka = 0 (Asym.) Ka = 0 (Asym.) A Sym. E Sym.
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Molecular Parameters for methyl butenyne and butynone
Inertia Ellipsoid for MBEY * qTOP = 59.2° Principal Axis (Asymmetric Limit) * qRAM = 35.7° * V3 = 706 cm-1 m r Axis (Gyroscope Limit) * S.L. Hsu, W.H. Flygare; J. Mol. Spec. 32 (1969) 375. Inertia Ellipsoid for Butynone m * qTOP = 62.3° Principal Axis (Asymmetric Limit) * qTOP = 36.8° * V3 = 375 cm-1 r Axis (Gyroscope Limit) * O.L. Stiefvater, J. Sheridan; Proc. Chem. Soc (Dec.) 368.
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Coalescence Phenomenon
B kr kf Lifetime Broadening Frequency Pulling Coalescence Narrowing No Reaction Increasing Reaction Rate
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Gyroscope Dynamics C: Coalescence Parameter
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Gyroscope Dynamics C: Coalescence Parameter N: Narrowing Parameter
(Friction)
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Gyroscope Coalescence
E Pentenyne 2D IR – CPFTMW Double Resonance Scan Gyroscope Coalescence J = 3 -2 J = 2 - 1
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Methylbutenyne Dynamic Rotational Spectrum
IR Prepares J=0 Exclusively through P(1) Excitation J = 1 - 0
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Vinyl Isocyanate Torsional Potential
Dynamic Rotational Spectroscopy State mixing Rigid rotor Justin L. Neill: WG08
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3164 cm-1 band Monitor 202101 R(1) Laser pumps
all three J = 21 a-type transitions at once; population in 101 of GS is much greater than that in 111 or 110, so most of excited population is in 202
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Conclusions and Acknowledgements
Intramolecular dynamics can be studied through line shape analysis of the rotational spectra of highly excited molecules Dynamic spectroscopy effects not limited to geometry changes Funding: NSF Experimental Physical Chemistry and NSF MRI Program
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Dynamic Rotational spectrum of molecules with sources of internal angular momentum
Methyl Butenyne rTOT = 99.8 states/cm-1 rABOVE = 13.5 12 Butynone rTOT = 31.4 states/cm-1 rABOVE = 12.7
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