Transition dipole moment

The transition dipole moment or transition moment, usually denoted d n m {displaystyle scriptstyle {mathbf {d} _{nm}}} for a transition between an initial state, m {displaystyle scriptstyle {m}} , and a final state, n {displaystyle scriptstyle {n}} , is the electric dipole moment associated with the transition between the two states. In general the transition dipole moment is a complex vector quantity that includes the phase factors associated with the two states. Its direction gives the polarization of the transition, which determines how the system will interact with an electromagnetic wave of a given polarization, while the square of the magnitude gives the strength of the interaction due to the distribution of charge within the system. The SI unit of the transition dipole moment is the Coulomb-meter (Cm); a more conveniently sized unit is the Debye (D). The transition dipole moment or transition moment, usually denoted d n m {displaystyle scriptstyle {mathbf {d} _{nm}}} for a transition between an initial state, m {displaystyle scriptstyle {m}} , and a final state, n {displaystyle scriptstyle {n}} , is the electric dipole moment associated with the transition between the two states. In general the transition dipole moment is a complex vector quantity that includes the phase factors associated with the two states. Its direction gives the polarization of the transition, which determines how the system will interact with an electromagnetic wave of a given polarization, while the square of the magnitude gives the strength of the interaction due to the distribution of charge within the system. The SI unit of the transition dipole moment is the Coulomb-meter (Cm); a more conveniently sized unit is the Debye (D). For a transition where a single charged particle changes state from | ψ a ⟩ {displaystyle |psi _{a} angle } to | ψ b ⟩ {displaystyle |psi _{b} angle } , the transition dipole moment (t.d.m.) {displaystyle { ext{(t.d.m.)}}} is where q is the particle's charge, r is its position, and the integral is over all space ( ∫ d 3 r {displaystyle int d^{3}mathbf {r} } is shorthand for ∭ d x d y d z {displaystyle iiint dx,dy,dz} ). The transition dipole moment is a vector; for example its x-component is In other words, the transition dipole moment can be viewed as an off-diagonal matrix element of the position operator, multiplied by the particle's charge. When the transition involves more than one charged particle, the transition dipole moment is defined in an analogous way to an electric dipole moment: The sum of the positions, weighted by charge. If the ith particle has charge qi and position operator ri, then the transition dipole moment is: For a single, nonrelativistic particle of mass m, in zero magnetic field, the transition dipole moment can alternatively be written in terms of the momentum operator, using the relationship This relationship can be proven starting from the commutation relation between position x and the Hamiltonian H: