Optical spectra of spatially oriented molecules: ICl in a strong electric field

Strong electric fields can hybridize rotational states of polar molecules and thus create pendular states in which the molecules are confined to librate over a limited angular range about the field direction. In this way, substantial spatial orientation can be attained for the lowest rotational states of many linear, symmetric and asymmetric top molecules. A large fraction of a molecular ensemble can often be condensed into these low rotational states by cooling in a supersonic expansion. Pendular eigenstates differ qualitatively from those of a rotor or an oscillator and can be observed spectroscopically; this provides a means to characterize the extent of the orientation achieved. Here we present high-resolution laser-induced fluorescence spectra of ICI A 3Π1â†� X 1Σ0 measured as a function of the electric field strength up to 36 kV cm–1. These spectra are compared with calculated transition frequencies and probabilities between pendulum/pinwheel states. The field-induced mixing of J states changes the transition probabilities markedly and enriches the spectra with many transitions that would be forbidden in the absence of the field. The transition probabilities fluctuate as the angular lobes of the two pendular wavefunctions involved come in and out of phase when the field strength is varied. The observed fluctuations are particularly pronounced in the present case because the dipole moment changes sign between the two electronic states.

[1]  H. Loesch,et al.  Reactive scattering from oriented molecules: The three‐center reaction K+ICl→KI+Cl, KCl+I , 1992 .

[2]  Sathyamurthy,et al.  State-resolved scattering of molecules in pendular states: ICl+Ar. , 1992, Physical review letters.

[3]  Miller Re,et al.  Spectroscopy of pendular states: The use of molecular complexes in achieving orientation. , 1992 .

[4]  Rost,et al.  Pendular states and spectra of oriented linear molecules. , 1992, Physical review letters.

[5]  H. Weiss,et al.  Monolayer structures of carbon monoxide adsorbed on sodium chloride: A helium atom diffraction study , 1991 .

[6]  H. Loesch,et al.  Reactive scattering of potassium from oriented and isotropic methyl iodide molecules , 1991 .

[7]  D. Herschbach,et al.  Alignment and orientation of rotationally cool molecules , 1991 .

[8]  E. E. Nikitin,et al.  Adiabatic channel potential curves for two linear dipole rotors. I. Classification of states and numerical calculations for identical rotors , 1991 .

[9]  D. Herschbach,et al.  Spatial orientation of molecules in strong electric fields and evidence for pendular states , 1991, Nature.

[10]  S. Stolte Aiming the molecular arrow , 1991, Nature.

[11]  E. Kryachko,et al.  Quantum rigid dipole in a permanent electric field. I. Rigorous treatment , 1991 .

[12]  K. Janda,et al.  Laser-induced fluorescence and microwave-optical double resonance spectra of the iodine chloride (A .rarw. X, 19 .rarw. 0) vibronic band: measurement of the chlorine atom hyperfine structure , 1990 .

[13]  H. Richardson,et al.  Infrared spectroscopy of CO on NaCl(100). II. Vibrational dephasing and band shapes , 1990 .

[14]  R. Levine,et al.  Dynamical aspects of stereochemistry , 1987 .

[15]  J. Thompson,et al.  Laser spectroscopy and microwave-optical double resonance of a supersonic expansion ICl A 3п (1) υ = 19 , 1983 .

[16]  A. Lübbert,et al.  Molecular beam focusing of ICl in rotational states with positive induced electric dipole moments , 1978 .

[17]  P. R. Brooks Reactions of Oriented Molecules , 1976, Science.

[18]  F. E. Cummings,et al.  Vibrational dependence of the dipole moment in the A3Π1 state of ICI , 1974 .

[19]  K. V. Meyenn Rotation von zweiatomigen Dipolmolekülen in starken elektrischen Feldern , 1970 .

[20]  R. Zare Calculation of Intensity Distribution in the Vibrational Structure of Electronic Transitions: The B3Π0+u—X1Σ0+g Resonance Series of Molecular Iodine , 1964 .

[21]  E. Condon The Franck-Condon Principle and Related Topics , 1947 .