Matrix Elements and the Wigner Eckhart Theorem Example: Difference between revisions
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(New page: Let <math> \vec J_1 </math> and <math> \vec J_2 </math> be two angular momentum operators, <math> \vec J = \vec J_1 + \vec J_2 </math> is the sum of these two vectors, and <math> |J M \ran...) |
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Let <math> \vec J_1 </math> and <math> \vec J_2 </math> be two angular momentum operators, <math> \vec J = \vec J_1 + \vec J_2 </math> is the sum of these two vectors, and <math> |J M \rangle </math> denotes the eigen states of <math> \vec J^2 </math> and <math> \bold J _z </math>. | Let <math> \vec J_1 </math> and <math> \vec J_2 </math> be two angular momentum operators, <math> \vec J = \vec J_1 + \vec J_2 </math> is the sum of these two vectors, and <math> |J M \rangle </math> denotes the eigen states of <math> \vec J^2 </math> and <math> \bold J _z </math>. | ||
<math> \bold (a) </math> Show that the matrix elements of <math> J_1^- , \langle J M | J_1^- | J' (M + 1)\rangle </math>, vanish, unless <math> \bold J' = \bold J </math> or <math> \bold J' = \bold J \pm 1 </math>. | |||
<math> \bold (b) </math> Show also that the following expressions are independent of <math> \bold M </math>: |
Latest revision as of 21:42, 5 April 2010
Let and be two angular momentum operators, is the sum of these two vectors, and denotes the eigen states of and .
Show that the matrix elements of , vanish, unless or .
Show also that the following expressions are independent of :