Coherent superposition of M-states in a single rovibrational level of H2 by Stark-induced adiabatic Raman passage

We prepare an ensemble of isolated rovibrationally excited (v = 1, J = 2) H-2 molecules in a phase-locked superposition of magnetic sublevels M using Stark-induced adiabatic Raman passage with linearly polarized single-mode pump (at 532 nm, similar to 6 ns pulse duration, 200 mJ/pulse) and Stokes (699 nm, similar to 4 ns pulse duration, 20 mJ/pulse) laser excitation. A biaxial superposition state, given by vertical bar psi(t)> = 1/root(2)[vertical bar v = 1, J = 2, M = -2 > - vertical bar v = 1, J = 2, M = +2 >], is prepared with linearly but cross-polarized pump and Stokes laser pulses copropagating along the quantization z-axis. The degree of phase coherence is measured by using the O(2) line of the H-2 E,F-X (0,1) band via 2 + 1 resonance enhanced multiphoton ionization (REMPI) at 210.8 nm by recording interference fringes in the REMPI signal in a time-of-flight mass spectrometer as the direction of the UV laser polarization is rotated using a half-wave plate. Nearly 60% population transfer from H-2 (v = 0, J = 0) ground state to the superposition state in H2 (v = 1, J = 2) is measured from the depletion of the Q(0) line of the E,F-X (0,0) band as the Stokes frequency is tuned across the (v = 0, J = 0) -> (v = 1, J = 2) Raman resonance. (C) 2014 AIP Publishing LLC.