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

• Published in: The Journal of chemical physics 2014-02, Vol.140 (7), p.074201-074201
• Main Authors: Mukherjee, Nandini, Dong, Wenrui, Zare, Richard N
• Format: Article
• Language: English
• Subjects: Adiabatic flow; Interference fringes; Ionization; Ions; Lasers; Linear polarization; Magnetic resonance; Phase coherence; Physics; Pulse duration; Recording; Superposition (mathematics); Ultraviolet lasers; Wave plates
• ISSN: 0021-9606; 1089-7690
• DOI: 10.1063/1.4865131

We prepare an ensemble of isolated rovibrationally excited (v = 1, J = 2) H2 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, ∼6 ns pulse duration, 200 mJ/pulse) and Stokes (699 nm, ∼4 ns pulse duration, 20 mJ/pulse) laser excitation. A biaxial superposition state, given by [line]ψ(t)⟩ = 1/√(2)[[line]ν = 1, J = 2, M = -2⟩ - [line]ν = 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 H2 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 H2 (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.