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![Page 1: Rotational dependence of intramolecular dynamics in acetylene as deduced from high resolution spectroscopy David Perry, Anthony Miller B. Amyay, A. Fayt,](https://reader035.fdocuments.net/reader035/viewer/2022062517/56649f095503460f94c1dc48/html5/thumbnails/1.jpg)
Rotational dependence of intramolecular dynamics in acetylene as deduced from high resolution spectroscopy
David Perry, Anthony Miller
B. Amyay, A. Fayt, and M. Herman
Fonds National de la Recherche Scientifique (Belgium)Action de Recherches Concertées de la Communauté française de Belgique
U. S. Department of Energy
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Outline
Acetylene rotation-vibration spectroscopy Polyad structure
Time-dependent dynamics Basic interactions Low-energy dynamics Intermediate energy dynamics
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Rotation-Vibration Spectroscopy of Acetylene
15,562 lines up to 8600 cm-1 fit to 0.001 cm-1
B. Amyay, S. Robert, M. Herman, A. Fayt, B. Raghavendra, A. Moudens, J. Thiévin, B. Rowe, and R. Georges, J. Chem. Phys. 131 (2009) 114301)
18,507 lines up to 13, 227 cm-1 fit to lower precision. IR, NIR, and THz data (B. Amyay, M. Herman, A. Fayt, L. Fusina, and A. Predoi-
Cross, Chem. Phys. Lett. 491 (2010) 17, and unpublished work)
369 constants 4 kinds of coupling terms:
anharmonic, vibrational l-type, rotational l-type, and Coriolis
Michel Herman Badr Amyay
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Acetylene vibrational modes
ν1 C-H stretch – symmetric 3374 cm-1
ν2 C C stretch 1974 cm-1
ν3 C-H stretch – asymmetric 3289 cm-1
ν4 trans bend 612 cm-1
ν5 cis bend 730 cm-1
Vibrational basis state labels: v1 v2 v3 v4 v5, l4 l5 e/f g/u
Total vibrational angular momentum: k = l4 +l5
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Polyad Structure of Acetylene
Based on the ratios of vibrational frequencies ν1 : ν2: ν3: ν4: ν5 = 5 : 3 : 5 : 1 : 1 Polyad number: Nr = 5v1+3v2+5v3+v4+v5 No. of stretch quanta: Ns = v1+v2+v3
Polyads without Coriolis coupling {Ns, Nr, ke/o, e/f, u/g, J}
Polyads with Coriolis coupling {Nr, e/f, u/g, J} 45 coupled states at 4,500 cm-1; 897 at 10,500 cm-1
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Time-dependent dynamics
n coupled levels:
If is the bright state, the spectral intensities are
The time-dependent wave function following a coherent excitation:
Probability of basis state j as a function of time:
Tony Miller
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Basic interactions: Rotational l-resonance
ν4 + ν5 at 1328 cm-1
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Basic interactions: Anharmonic (+ Rotational l-resonance)
ν3 at 3288 cm-1
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Basic interactions: More anharmonic couplings
Darling-Dennison bending resonance K4455
Crucial to bending dynamics and birth of new kinds of bending modes (Field, Kellman)
Darling-Dennison CH stretching resonance K1133
Responsible for normal to local mode transition (Lehmann)
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Basic interactions: Coriolis (+ Rotational l-res + anharmonic)
ν3 at 3288 cm-1
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Thermally rotationally averaged dynamics
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A stretch-bend combination near 4500 cm-1
ν3 + 2ν4 at 4498 cm-1
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A bending overtone near 4400 cm-1
7ν4 at 4419 cm-1
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Conclusions: Lower energy dynamics
Sparse coupling with quantum beats. An inhomogeneous thermal rotational average produces the
appearance of irreversible decay. The nature of the bright state is crucial.
similar behavior across polyads. Rotational l-resonance
dominates at high J. Coriolis coupling
localized and contributes little to overall dynamics
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Intermediate energies: A bending overtone near 10,500 cm-1
Polyad connects 897 vibrations
Jonathan Martens
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Strong rotational effects
Intermediate energies: A bending overtone near 10,500 cm-1
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Exploration
of phase space
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Conclusions: Intermediate energy region
Dynamics span 3 orders of magnitude in time. A hierarchy of coupling stages.
The volume of phase space explored increases dramatically with rotational excitation.
The nature of the bright state remains crucial.