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6  Transition Metal Solid-state lasers   37

                    rule and the Laporte selection rule. According to the spin selection rule, a transi-
                    tion can only occur between levels in which the number of unpaired electrons in
                    the initial and final levels is the same. In cases where a single electron undergoes
                    a transition, the spin must be the same for the initial and final levels. According
                    to one formulation of  the  Laporte  selection  rule,  a transition  is  forbidden  if  it
                    involves only a redistribution of electrons having similar orbitals v, ithin a single
                    quantum  shell.  This  formulation  is  particularly  relevant  to  transition  metals
                    because transitions  tend to be between  different  3d  levels but within  the same
                    quantum shell. For example, transitions involving only a rotary charge displace-
                    ment in one plane would be forbidden by this selection rule.
                        Selection  rules  were  also  considered  by  Tanabe and  Sugano. Usually  the
                    strong interaction that allows a transition between levels with the emission of a
                    photon is the electric dipole interaction. However, for the 3d electrons, all transi-
                    tions between the various levels are forbidden since all levels have the same par-
                    ity. Consequently, three other transition interactions were considered: the electric
                    dipole interaction  coupled  with a vibration,  the electric  quadrupole interaction,
                    and the magnetic  dipole interaction. The strengths of these various interactions
                    LA ere estimated. From these estimations. it was concluded that the electric dipole
                    transition coupled with vibration, that is, a vibronic transition, u as the strongest
                    interaction. Vibronic transitions involve emission or absorption of a photon and a
                    quantized 3mount of lattice vibrations referred to as a phonon. Vibronic interac-
                    tions  were estimated  to be  about 2 orders  of magnitude  stronger than the nexl
                    strongest interaction, the magnetic dipole interaction.
                        McCumber  [ 101 investigated the absorption  and emission that results from
                    vibromc  interactions. Terminology used in the original paper refers to phonon-
                    terminated absorption and emission rather than vibronic transitions. McCumber
                    analyzed the absorption, emission. and gain of the transition metal Ni in the ini-
                    tial paper. Emission spectra from Ni:MgF,  were characterized by sharp emission
                    lines  and  a  broad  emission  spectra  on  &e  long-wavelength  side  of  the  sharp
                    emission lines.  Sharp lines were associated nith electronic transitions, whereas
                    the  long-wavelength  emission  was  associated  with  vibronic  emission.  Since
                    then. this general analysis has been extended to many of the transition metals.
                        Through the use of an analysis similar to the McCumber analysis, the gain
                    characteristics  of  an active atom can be related  to the  absorption  and emission
                    spectra. Relating the gain to the absorption and emission spectra is of consider-
                    able practical importance since the  gain as a function of wavelength is  a more
                    difficult measurement  than the absorption  and emission.  Emission  and absorp-
                    tion  spectra often  display relatively  sharp electronic, or no phonon.  transitions
                    accompanied by adjacent broad vibronic transitions associated with the emission
                    and absorption of phonons. General absorption and emission processes appear in
                    Fig.  8. At  reduced  temperatures  only  phonon  emission  is  observed  since  the
                    average  phonon  population  is  low.  In  this  case.  the  vibronic  emission  spectra
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