Thursday, September 22, 2011

electric dipole

Dipole Moment

The electric dipole moment for a pair of opposite charges of magnitude q is defined as the magnitude of the charge times the distance between them and the defined direction is toward the positive charge. It is a useful concept in atoms and molecules where the effects of charge separation are measurable, but the distances between the charges are too small to be easily measurable. It is also a useful concept in dielectrics and other applications in solid and liquid materials.
Applications involve the electric field of a dipole and the energy of a dipole when placed in an electric field. 

Electric dipole transition is the dominant effect of an interaction of an electron in an atom with the electromagnetic field.
Following , consider an electron in an atom with quantum Hamiltonian H0, interacting with a plane electromagnetic wave
 {\mathbf E}({\mathbf r},t)=E_0 {\hat{\mathbf z}} \cos(ky-\omega t), \ \ \ {\mathbf B}({\mathbf r},t)=B_0{\hat{\mathbf x}} \cos(ky-\omega t).
Write the Hamiltonian of the electron in this electromagnetic field as
 H(t) \ = \ H_0 + W(t).
Treating this system by means of time-dependent perturbation theory, one finds that the most likely transitions of the electron from one state to the other occur due to the summand of W(t) written as
 W_{DE}(t) = \frac{q E_0}{m\omega}  p_z \sin \omega t. \,
Electric dipole transitions are the transitions between energy level in the system with the Hamiltonian H0 + WDE(t).
Between certain electron states the electric dipole transition rate may be zero due to selection rule, and then the transitions between such levels are approximated by higher-order transitions.
The next order summand in W(t) is written as
 W_{DM}(t) = \frac{q}{2m} (L_x + 2S_x) B_0 \cos \omega t \,
and describes magnetic dipole transitions.
Even smaller contributions to transition rates are given by higher electric and magnetic multipole transitions

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