1) degenerate parametric amplification
简并参量放大
1.
A new analytical solution for the phase-mismatched Fokker-Planck equation of degenerate parametric amplification, and its application in evaluation of the amplitude quantum fluctuation after passing through the quasi-phase-matching(QPM) device is presented.
在前文的基础上求得了简并参量放大系统在位相不匹配情况下的Fokker_Planck方程一个新的解析解,然后通过准位相匹配(QPM),计算振幅的量子起伏。
2) non-degenerate parametric amplification
非简并参量放大
1.
Optimum realization of the EPR paradox in the non-degenerate parametric amplification system;
在非简并参量放大系统中EPR佯谬的最佳实现
3) Degenerate parametric amplifier
简并参量放大器
4) degenerate optical parametric amplifier
简并光学参量放大器
5) nondegenerate optical parametric amplifier
非简并光学参量放大器
1.
The bright Einstein-Podolsky-Rosen(EPR) beam (with quantum correlations between the quadrature-phase amplitudes of the spatially separated signals and the idler beams), and the bright two-mode quadrature squeezed light have been experimentally generated from a cw nondegenerate optical parametric amplifier (NOPA) injected by seed wave with degenerate frequency but orthogonal polarization.
通过非简并光学参量放大器获得了明亮双模正交压缩光及明亮EPR光束 。
6) non-degenerate optical parametric amplification
非简并光学参量放大
1.
In this paper, we present the analytical solution of the Fokker-Planck equation of non-degenerate optical parametric amplification(NOPA)for generation of squeezed light.
通过解非简并光学参量放大的Fokker Planck方程 ,得出压缩态光的腔内最大压缩的量子起伏为 1 16 (真空起伏为 1 4 ) ,与已知的简并光学参量放大情形腔内最大压缩为 1 8相比 ,压缩度提高了一倍 。
补充资料：断简
1.见"断简残编"。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条