Page 352 - Instant notes
P. 352

Physical Chemistry     338


           A characteristic feature of a molecule that phosphoresces is that it possesses an excited
        triplet electronic state,  T 1, of energy similar to the excited singlet state,  S 1, and into
        which the excited singlet state can convert. In a triplet state two electrons in different
        orbitals have parallel spins ( ). Although normally forbidden, if a mechanism exists for
        converting paired ( ) electron spins into unpaired ( ) electron spins the excited S1
        state may undergo  intersystem  crossing  into the  T 1 state. (The usual mechanism for
        intersystem crossing is spin-orbit coupling in which the magnetic field from the nucleus
        of  a  heavy  atom  induces  a neighboring electron to flip its spin orientation.) After
        intersystem crossing the molecule continues to step down the vibrational ladder of the T 1
        state by loss of energy in collisions with surrounding molecules. The molecule cannot
        lose electronic energy by radiative transfer to the ground state because a triplet-singlet
        transition is forbidden. However, the transition is not entirely forbidden because the same
        mechanism that permits singlet to triplet  intersystem crossing in the first place also
        breaks the selection rule so that the molecules are able to emit weak phosphorescence
        radiation on a longer timescale.


                                Photoelectron spectroscopy

        The absorption of a photon of high enough energy may cause an electron to be ejected
        entirely from a molecule. In photoelectron spectroscopy, molecules are irradiated with
        high frequency, monochromatic light and the kinetic energy of the emitted photoelectrons
        is analyzed. The resulting photoelectron spectrum provides  information  on  the  energy
        levels of the orbitals from which the electrons were emitted. Conservation  of  energy
        dictates that if the incoming photon has frequency, v, and the ionization energy for the
        electron in an orbital is I, the kinetic energy of the emitted photoelectron is:




        The  kinetic  energy of the electrons is determined from the strength of the electric or
        magnetic field required to bend their path into a detector. The slower the ejected electron,
        the  lower in energy the molecular orbital from which it was ejected. Ultraviolet
        photoelectron spectroscopy provides information on the energy levels of the molecular
        orbitals of the  valence electrons  of  molecules; X-ray photoelectron spectroscopy
        provides information on the energy levels of  core electrons. If the apparatus has
        sufficient resolution of photoelectron kinetic energy, it may be possible to resolve fine
        structure  in  the  photoelectron  spectrum associated with the vibrational levels of the
        molecular cation formed by the ionization.
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