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Nuclear magnetic resonance energy separation/splitting

NMR nuclear magnetic resonance spectroscopy, non-degenerate orbitals atomic orbitals that have been split to occupy slightly different energy levels, non-polar (molecule) a molecule with no separation of charge it will not be attracted to a positive or negative charge. [Pg.492]

Lichten [3 5] studied the magnetic resonance spectrum of the para-H2, N = 2 level, and was able to determine the zero-field spin-spin and spin-orbit parameters we will describe how this was done below. Before we come to that we note, from table 8.6, that in TV = 2 it is not possible to separate Xo and X2. Measurements of the relative energies of the J spin components in TV = 2 give values of Xo + fo(iX2, and the spin-orbit constant A the spin rotation constant y is too small to be determined. In figure 8.18 we show a diagram of the lower rotational levels for both para- and ortho-H2 in its c3 nu state, which illustrates the difference between the two forms of H2. This diagram does not show any details of the nuclear hyperfine splitting, which we will come to in due course. [Pg.436]


See other pages where Nuclear magnetic resonance energy separation/splitting is mentioned: [Pg.376]    [Pg.193]    [Pg.24]    [Pg.434]    [Pg.131]    [Pg.138]    [Pg.436]    [Pg.450]    [Pg.57]    [Pg.18]    [Pg.379]    [Pg.374]    [Pg.140]    [Pg.12]    [Pg.256]    [Pg.186]   
See also in sourсe #XX -- [ Pg.54 ]




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