This transition moment type must
      be used for multiphoton or 
Raman
      transitions. It is also appropriate for single photon transitions
      classified as parallel or perpendicular. The notation used here is
      slightly non-standard; the 
Strength
      numbers are actually taken as the sum and difference of the
      two components such that the value of the vibronic matrix element
      where 
K increases is
      (taking 
q > 0):
      
 <stateA
, 
K+
q| 
μ| stateB
,
        
K> = 
T(
k,
q) + 
T(
k,
-q)
        
and where it decreases is:
           <stateA, K-q| μ| stateB, K> = T(k,q) - T(k,-q)
        (
k,
q) and 
T(
k,
-q) are the 
Strength parameters; they are not necessarily
      symmetry related and two numbers are in general required for 
q ≠ 0. With this
      definition the operators multiplying 
T(
k,
q) and 
T(
k,
-q)
      will have often have different symmetries in more symmetric point
      groups (such as C
2v), so only one may be required. For
      
k = 1 the following identifications can be made:
      
<stateA|z|stateB> = T(1,0)
        <stateA|x|stateB> = -2½T(1,-1)
        <stateA|y|stateB> = i 2½T(1,1)
      
      making the three possible components approximately equivalent to
      the three Cartesian components, but with a different phase choice.
      
 
      While the sign or phase of transition moment matrix elements is
      often irrelevant, it will be important if more than one transition
      moment can contribute to a given transition, either through
      multiple components for a single vibronic transition, or if
      different vibronic states are mixed, allowing interference between
      different pathways to the same final state. In such circumstances
      the relative signs are important and, given the definition above,
      the order in which states are specified will make a difference to
      the parameters required. Swapping the bra and ket over will change
      the sign of the 
T(
k,
-q) component.