Infrared—ultraviolet double resonance measurements on the relaxation of rotational energy in the (31, 214151) Fermi resonance states of C2H2

[1]  B. Orr,et al.  Rotationally resolved V–V transfer in C2D2/Ar collisions: Characterization of a vibrational bottleneck , 1991 .

[2]  H. Zacharias,et al.  Direct measurements of collision-induced state-to-state rotational energy transfer rates in C2H2 (ν″2 = 1) , 1991 .

[3]  Ian W. M. Smith,et al.  Tunable infrared–tunable ultraviolet double-resonance experiments on HCN , 1991 .

[4]  C. Bewick,et al.  Rotationally specific mode–to–mode vibrational energy transfer in D2CO/D2CO collisions. I. Spectroscopic aspects , 1990 .

[5]  R. Farrow,et al.  Pump–probe measurements of state‐to‐state rotational energy transfer rates in N2 (v=1) , 1990 .

[6]  B. Orr,et al.  Raman‐ultraviolet optical double resonance spectroscopy in gas‐phase acetylene , 1989 .

[7]  A. L. Utz,et al.  Collisional relaxation of single rotational states in highly vibrationally excited acetylene , 1988 .

[8]  J. Haub,et al.  Coriolis‐assisted vibrational energy transfer in D2CO/D2CO and HDCO/HDCO collisions: Experiment and theory , 1987 .

[9]  J. Haub,et al.  Mode-to-mode vibrational energy transfer in D2CO: Evidence of coriolis-enhanced rotational selectivity , 1984 .

[10]  M. Loy,et al.  Measurement of absolute state‐to‐state rate constants for collision‐induced transitions between spin‐orbit and rotational states of NO(X 2Π, v = 2) , 1982 .

[11]  M. Loy,et al.  State-to-state rotational and electronic collisional relaxation study of nitric oxide , 1981 .

[12]  A. Schenzle,et al.  Optical coherent transients: Generalized two-level solutions , 1976 .

[13]  K. Innes.  Analysis of the Near Ultraviolet Absorption Spectrum of Acetylene , 1954 .