HW 03: Difference between revisions
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|<math>\int_{-\infty}^{\infty} \sum _n a_n \phi_n (t) \sum _m |
|<math>\int_{-\infty}^{\infty} \sum _n a_n \phi_n (t) \sum _m b_m \phi_m (t)^* \,dt</math> |
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|<math>=\sum_n \sum _m a_n b_m^* \int_{-\infty}^{\infty} \phi_n (t) \phi_m (t)^* \,dt</math> |
|<math>=\sum_n \sum _m a_n b_m^* \int_{-\infty}^{\infty} \phi_n (t) \phi_m (t)^* \,dt</math> |
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|<math>=\sum_n \sum _m a_n b_m^* \left \langle \phi_n (t) | \phi_m (t) |
|<math>=\sum_n \sum _m a_n b_m^* \left \langle \phi_n (t) | \phi_m (t) \right \rangle</math> |
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|<math>=\sum_n \sum _m a_n b_m^* \delta_{nm |
|<math>=\sum_n \sum _m a_n b_m^* \delta_{nm}</math> |
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|<math>=\sum_n a_n b_n^*</math> |
|<math>=\sum_n a_n b_n^*</math> |
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{| border="0" cellpadding="0" cellspacing="0" |
{| border="0" cellpadding="0" cellspacing="0" |
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|<math>\int_{-\infty}^{\infty} \sum _n a_n \phi_n (t) \sum _m |
|<math>\int_{-\infty}^{\infty} \sum _n a_n \phi_n (t) \sum _m a_m \phi_m (t)^* \,dt</math> |
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|<math>=\sum_n \sum _m a_n |
|<math>=\sum_n \sum _m a_n a_m^* \int_{-\infty}^{\infty} \phi_n (t) \phi_m (t)^* \,dt</math> |
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|<math>=\sum_n \sum _m a_n |
|<math>=\sum_n \sum _m a_n a_m^* \left \langle \phi_n (t) | \phi_m (t) \right \rangle</math> |
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|<math>=\sum_n \sum _m a_n |
|<math>=\sum_n \sum _m a_n a_m^* \delta_{nm}</math> |
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|<math>=\sum_n a_n |
|<math>=\sum_n \left | a_n \right |^2</math> |
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Latest revision as of 17:27, 12 November 2008
Problem
If and span the space of functions for which and are members and and , then show
Notes
- This notation is called the Bra Ket , or Dirac notation. It denotes the inner product.