bound electron 束缚电子 $ M0 @& k: ]! S; E4 ~# s
bound electron hole 束缚电子空穴 2 w/ M z6 }/ m* e3 ?3 K4 h
bound hole 束缚空穴 9 J! b; s4 I: u
bound mode 束缚模 * I4 N, F7 L0 o2 Z9 ]( _2 v9 ~
bound scattering 束缚散射
0 q3 Y" Z, F+ m3 Q9 {' | S) o1 fboundary scattering 边界散射 / R6 a1 L, M& L! b) T
boundary surface 界面
. m/ P) i/ m* I% q5 Aboundary wave 边界波 + c3 M: X, S4 }' }& N: I/ o! x
bounded matrix 有界矩阵 ' j6 X; e* O# H
bounded operator 有界算子 ! `+ h. B7 ]4 R2 R- c
bounded projection 有留投影
7 n5 i$ E3 P3 m3 hbouteillenstein 暗绿玻璃bound state 束缚[能]态 3 ^* h& x7 _* H
bound-bound laser 束缚–束缚激光器
4 M/ `. z( |) E: N/ p9 m5 g; k) ~bound-bound transition 束缚–束缚跃迁
; R( p" ^2 O: Q0 k+ a+ Qbound-free laser 束缚–自由激光器，分子缔合激光器 : \% {8 k! N+ ]# P" {
bound-free transition 束缚–自由跃迁 ( M$ `" l, ^% c+ n% V
boundary condition 边界条件 8 f9 l8 C, n$ C% `
boundary diffraction 边界衍射 ; |+ V* ], D3 p: m
boundary layer 界面层 |
发表于 2012-8-14 22:56:05
