论文部分内容阅读
高功率激光与“神光”装置
【出 处】
：
激光与光电子学进展
【发表日期】
：
1991年28期
其他文献
Time-division multiplexing holographic display using angular-spectrum layer-oriented method (Invited
A time-division multiplexing method for computer-generated holograms (CGHs) is proposed to solve the problem of the limited space-bandwidth product. A three-dimensional (3-D) scene is divided into multiple layers at different depths. The CGH corresponding
采用飞秒钛宝石激光放大器二次谐波为泵浦源,行波泵浦BBO晶体光参量放大器,获得了可调谐输出(0.44～2.6 μm),最大输出能量约40 μJ/脉冲,测量了参量激光的调谐特性、能量分布和线宽,理论与实验符合较好。
A new compensation method for temperature-dependent gain tilt in L-band EDFA by adjusting only inser
A novel compensation method for temperature-dependent gain tilt of L-band erbium-doped fiber amplifier (L-EDFA) is proposed, in which the attenuation between stages is the only parameter to be adjusted. A simple linear relationship between the attenuation
Broadband mid-infrared second harmonic generation using epitaxial polydomain barium titanate thin fi
The mid-infrared (mid-IR) second-order optical nonlinearity of the barium titanate (BTO) thin films was characterized by second harmonic generation (SHG). The epitaxial BTO thin films were grown on strontium titanate substrates by pulsed-laser deposition.
期刊
We propose and experimentally demonstrate a 2 × 2 imaging multiple-input–multiple-output (MIMO) Nyquist single carrier visible light communication (VLC) system based on spectral efficient 64/32-ary quadrature amplitude modulation, as well as pre- and post
2-Aminoethyldiphenyl borate (2-APB) is the most commonly used pharmacological agent in the study of calcium release-activated channels (CRACs); however, its inhibitory mechanism to CRACs remains unclear. To address this issue, we systematically employed c
The influence of optical breakdown on stimulated Brillouin scattering (SBS) process is investigated with purified CCl4, acetone, and CS2 mediums which are obtained through 0.22-μm pore-size filter. Experiments are conducted with a Nd:YAG Q-switched laser
This paper has solved the Chester modified heat conduction equation of the different relaxation time τ value under different temperature conditions, different boundary conditions and the different initial conditions by different means of methods. These so