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 
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)
         
       
      T(
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.
      
      While the sign 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.