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http://en.wikipedia.org/wiki/Hermitian_adjoint Suppose H is a Hilbert space, with inner product . Consider a continuous linear operator A : H → H (this is the same as a bounded operator). Using the Riesz representation theorem, one can show that there exists a unique continuous linear operator A* : H → H with the following property: <Ax,y> = <x,A*y> This operator A* is the adjoint of A. This can be seen as a generalization of the adjoint matrix of a square matrix which has a similar property involving the standard complex inner product. 也就是說 <Av|u> = <v|A*u> 這個式子本身就是A*的定義 因此 <u|A|u> = <u|Au> = <u|(A*)*u> = <A*u|u> ※ 引述《chris80634 (紛飛)》之銘言: : 令波函數為u(x) : <u|A|u> = <A*u|u> : 為什麼A拿到bra那邊的時候會變成共軛? : 我有想過會不會是因為他要對u*(x)作用 : 所以他本身也要是一個共軛的算符? : 以上 : 感謝解答 -- ※ 發信站: 批踢踢實業坊(ptt.cc) ◆ From: 61.57.113.89
realtemper:推~內積的基本定義~ 12/26 01:11