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Angular momentum, tunneling rotation

Fig. 12.5. Zeroth-order potentials Veff(R-,j,Sl,J) defined in (12.7) for fl = 0 and several total angular momentum quantum numbers J. The excited rotational states can decay either by tunneling (shape resonances) or by rotational predissociation ( Feshbach resonances) as indicated by the horizontal arrows. The excitation through the IR photon originates from the vibrational ground state n = 0 which is not shown in the figure. Fig. 12.5. Zeroth-order potentials Veff(R-,j,Sl,J) defined in (12.7) for fl = 0 and several total angular momentum quantum numbers J. The excited rotational states can decay either by tunneling (shape resonances) or by rotational predissociation ( Feshbach resonances) as indicated by the horizontal arrows. The excitation through the IR photon originates from the vibrational ground state n = 0 which is not shown in the figure.
See other pages where Angular momentum, tunneling rotation is mentioned: [Pg.379]    [Pg.103]    [Pg.40]    [Pg.219]    [Pg.185]    [Pg.60]    [Pg.60]    [Pg.5]    [Pg.39]    [Pg.553]    [Pg.416]    [Pg.34]    [Pg.34]    [Pg.135]   
See also in sourсe #XX -- [ Pg.219 , Pg.220 , Pg.221 ]



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Angular momentum

Angular momentum rotation

Angular momentum rotational

Rotational momentum

Rotational tunneling

Rotational tunnelling

Tunneling rotation

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