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Eigenstates molecular photonics, quantum

To see the origin of the molecular phase lag in the one- vs. three-photon control scenario, we reconsider the formalism discussed in Section 3.3.2. However, for notational simplicity, we denote the set of scattering eigenstates of the full Hamiltonian at energy E and fragment quantum numbers n in channel q as E, n ), that is, we subsume the q within the labels n. [Pg.135]


See other pages where Eigenstates molecular photonics, quantum is mentioned: [Pg.413]    [Pg.238]    [Pg.214]    [Pg.512]    [Pg.215]    [Pg.120]    [Pg.331]    [Pg.292]    [Pg.12]    [Pg.260]    [Pg.22]    [Pg.128]   


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Eigenstate

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