A relaxation-assisted 2D IR spectroscopy method

  1. Dmitry V. Kurochkin,
  2. Sri Ram G. Naraharisetty, and
  3. Igor V. Rubtsov
  1. Department of Chemistry, Tulane University, New Orleans, LA 70118
  1. Edited by F. Fleming Crim, University of Wisconsin, Madison, WI, and approved April 13, 2007 (received for review January 22, 2007)

  1. Fig. 1.

    Structure of 3-cyanocoumarin. The transition moment directions of the modes involved in this study are shown by arrows.


  2. Fig. 2.

    Linear spectrum of 3-cyanocoumarin and the spectra of the IR pulses tuned to match the CN and CO bands.


  3. Fig. 3.

    Two-dimensional IR absorptive spectra of cyanocoumarin measured at T-delays of 670 fs (A), 2 ps (B), and 4 ps (C). The zero-contour ωt z frequencies are shown. In B Inset, the amplitude of the upper-left part of the spectrum was multiplied by a factor of 3.


  4. Fig. 4.

    Energy diagram (A) and rephasing Liouville pathways describing the direct-coupling (B and C) and relaxation-assisted (C and D) cross-peaks.


  5. Fig. 5.

    CO (A) and CC (C) peak amplitudes and CO (B) and CC (D) peak frequencies as a function of T-delay, obtained from the dual-frequency (ωt, T) spectrum. The heavy line represents the results of global modeling with the following parameters: k CN/CO = (30 ps)−1, k CN/CC = (4.3 ps)−1, k CN/X = (7.9 ps)−1, k CN/gr = (3.7 ps)−1, k CO/CC = (2.5 ps)−1, k CO/X = (3.6 ps)−1, k CO/gr = (4.8 ps)−1, k CC/X = (7.6 ps)−1, k CC/gr = (8.2 ps)−1, k X/gr = (27.6 ps)−1, ΔCO/CN = 2 ± 0.5 cm−1, ΔCN/CC = 12 ± 3 cm−1, ΔCO/CC = 0.9 ± 0.2 cm−1, ΔX/CO = 0.4 ± 0.1 cm−1, ΔCC/X = 18 ± 0.2 cm−1, ΔCO = 14 ± 1.5 cm−1, ΔCC = 17 ± 2 cm−1, and E X = 1,420 cm−1.


  6. Fig. 6.

    CO peak amplitude for AcPhCN as a function of T-delay, obtained from the (ωt, T) dual-frequency spectra.


  7. Fig. 7.

    RA 2DIR absorptive spectrum of AcPhCN, measured at T = 11 ps.


  8. Fig. 8.

    Schematic representation of fundamental vibrational states as a function of their location in a molecule. Horizontal bars show spatial extent of vibrational modes.


  9. Fig. 9.

    Pulse geometry for the dual-frequency 2D IR experiments with the k 1 and k 2 pulses centered at 4 μm and the k 3 and LO pulses centered at 6 μm.


Footnotes

  • To whom correspondence should be addressed. E-mail: irubtsov{at}tulane.edu
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