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The “bound wavefunction” on the repulsive excited ( ) state of the HD+ molecule
Authors:Wei Gao  Bin‐Bin Wang  Xue‐Jin Hu  Yong‐Chang Han
Affiliation:Department of Physics, Dalian University of Technology, Dalian, China
Abstract:The time‐independent Schrödinger equation for the HD+ molecule is solved beyond the Born–Oppenheimer (B‐O) approximation. In the adiabatic representation, the wavefunction of the ground vibrational eigenstate is found to contain two parts: One is on the ground urn:x-wiley:00207608:media:qua25394:qua25394-math-0003 ( urn:x-wiley:00207608:media:qua25394:qua25394-math-0004) state which is dominant, and the other is on the repulsive excited urn:x-wiley:00207608:media:qua25394:qua25394-math-0005 ( urn:x-wiley:00207608:media:qua25394:qua25394-math-0006) state in the range from R = 0.0 to R = 5.0 Bohr. This is because the nonadiabatic coupling between the ground urn:x-wiley:00207608:media:qua25394:qua25394-math-0007 ( urn:x-wiley:00207608:media:qua25394:qua25394-math-0008) and excited urn:x-wiley:00207608:media:qua25394:qua25394-math-0009 ( urn:x-wiley:00207608:media:qua25394:qua25394-math-0010) states is strong in that region. The influences of the nonadiabatic coupling on the vibrational eigenfunctions are discussed in detail.
Keywords:Born–  Oppenheimer approximation  nonadiabatic interaction  the HD+ molecule  vibrational eigenstate
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