HW 03: Difference between revisions
		
		
		
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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 b_m \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> | |<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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| |} | |} | ||
| {| border="0" cellpadding="0" cellspacing="0" | |||
| <math>\int_{-\infty}^{\infty} \sum _n a_n \phi_n (t) \sum  | |- | ||
| |<math>\int_{-\infty}^{\infty} \sum _n a_n \phi_n (t) \sum _m a_m \phi_m (t)^* \,dt</math> | |||
| |<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 a_m^* \left \langle \phi_n (t) | \phi_m (t) \right \rangle</math> | |||
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| |<math>=\sum_n \sum _m a_n a_m^* \delta_{nm}</math> | |||
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| |<math>=\sum_n \left | a_n \right |^2</math> | |||
| |} | |||
Latest revision as of 18:27, 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.