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Figure8_NALM-master 1

于 2021-02-20 发布 文件大小:97KB
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  NALM锁模激光器仿真，非线性环路反射镜锁模获得飞秒激光脉冲。(The simulation of NALM mode-locked laser shows that the femtosecond laser pulse can be obtained by mode-locked non-linear loop mirror.)

文件列表：

Figure8_NALM-master 1, 0 , 2019-03-06
Figure8_NALM-master 1\.DS_Store, 8196 , 2019-03-06
__MACOSX, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\._.DS_Store, 120 , 2019-03-06
Figure8_NALM-master 1\.gitattributes, 378 , 2016-06-08
Figure8_NALM-master 1\.gitignore, 670 , 2016-06-08
Figure8_NALM-master 1\Amplifier, 0 , 2019-03-05
Figure8_NALM-master 1\Amplifier\.DS_Store, 6148 , 2019-03-05
__MACOSX\Figure8_NALM-master 1\Amplifier, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\Amplifier\._.DS_Store, 120 , 2019-03-05
Figure8_NALM-master 1\Amplifier\AmpSimp, 0 , 2019-03-05
Figure8_NALM-master 1\Amplifier\AmpSimp\.DS_Store, 6148 , 2019-03-05
__MACOSX\Figure8_NALM-master 1\Amplifier\AmpSimp, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\Amplifier\AmpSimp\._.DS_Store, 120 , 2019-03-05
Figure8_NALM-master 1\Amplifier\AmpSimp\AmpSimpNoise.m, 1733 , 2016-06-08
Figure8_NALM-master 1\Amplifier\AmpSimp\AmpSimpNonoise.m, 638 , 2016-06-08
Figure8_NALM-master 1\Amplifier\AmpSimp\filter_lorentz_tf.m, 673 , 2016-06-08
Figure8_NALM-master 1\Amplifier\AmpSimp\gain_saturated2.m, 549 , 2016-06-08
Figure8_NALM-master 1\Amplifier\AmpSimp\gain_saturated3.m, 496 , 2016-06-08
Figure8_NALM-master 1\Amplifier\AmpSimp\testcodes, 0 , 2016-06-08
Figure8_NALM-master 1\Amplifier\AmpSimp\testcodes\test_fzero.m, 250 , 2016-06-08
Figure8_NALM-master 1\Amplifier\AmpSimp\testcodes\test_gain_saturated.m, 374 , 2016-06-08
Figure8_NALM-master 1\Amplifier\AmpSimp\testcodes\test_onetrip_gain.m, 1019 , 2016-06-08
Figure8_NALM-master 1\Amplifier\AmpSimp\testcodes\test_Pin_Pout.m, 493 , 2016-06-08
Figure8_NALM-master 1\Amplifier\testcodes, 0 , 2016-06-08
Figure8_NALM-master 1\Amplifier\testcodes\Amplifier_test.m, 3094 , 2016-06-08
Figure8_NALM-master 1\Amplifier\testcodes\plotall.m, 722 , 2016-06-08
Figure8_NALM-master 1\Amplifier\testcodes\plotsimp.m, 864 , 2016-06-08
Figure8_NALM-master 1\Coupler, 0 , 2016-06-08
Figure8_NALM-master 1\Coupler\coupler.m, 355 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master, 0 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\.DS_Store, 6148 , 2019-03-06
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\._.DS_Store, 120 , 2019-03-06
Figure8_NALM-master 1\Figure8_NALM-master\.gitattributes, 378 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\.gitignore, 670 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\Amplifier, 0 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\.DS_Store, 6148 , 2019-03-05
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\Amplifier, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\._.DS_Store, 120 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\AmpSimp, 0 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\AmpSimp\.DS_Store, 6148 , 2019-03-05
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\AmpSimp, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\AmpSimp\._.DS_Store, 120 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\AmpSimp\filter_lorentz_tf.m, 673 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\AmpSimp\gain_saturated2.m, 549 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\testcodes, 0 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\testcodes\.DS_Store, 6148 , 2019-03-05
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\testcodes, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\testcodes\._.DS_Store, 120 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\Amplifier\testcodes\plotsimp.m, 864 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\Coupler, 0 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\Coupler\.DS_Store, 6148 , 2019-03-05
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\Coupler, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\Coupler\._.DS_Store, 120 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\Coupler\coupler.m, 355 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\filter, 0 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\filter\filter_gauss.m, 785 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\GNLSE, 0 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\GNLSE\.DS_Store, 6148 , 2019-03-05
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\GNLSE, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\GNLSE\._.DS_Store, 120 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\GNLSE\Solvers, 0 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\GNLSE\Solvers\.DS_Store, 6148 , 2019-03-05
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\GNLSE\Solvers, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\GNLSE\Solvers\._.DS_Store, 120 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\GNLSE\Solvers\IP_CQEM_FD.m, 4823 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\GNLSE\Solvers\Linearoperator_w.m, 409 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\GNLSE\Solvers\NonLinearoperator_w.m, 952 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\GNLSE\Solvers\Raman_response_w.m, 793 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\main2.m, 6405 , 2019-03-05
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\._main2.m, 120 , 2019-03-05
Figure8_NALM-master 1\Figure8_NALM-master\main3.m, 7562 , 2016-06-08
Figure8_NALM-master 1\Figure8_NALM-master\Utility, 0 , 2019-03-06
Figure8_NALM-master 1\Figure8_NALM-master\Utility\.DS_Store, 6148 , 2019-03-06
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\Utility, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\Figure8_NALM-master\Utility\._.DS_Store, 120 , 2019-03-06
Figure8_NALM-master 1\filter, 0 , 2016-06-08
Figure8_NALM-master 1\filter\filter_gauss.m, 785 , 2016-06-08
Figure8_NALM-master 1\GNLSE, 0 , 2019-03-05
Figure8_NALM-master 1\GNLSE\.DS_Store, 6148 , 2019-03-05
__MACOSX\Figure8_NALM-master 1\GNLSE, 0 , 2019-03-08
__MACOSX\Figure8_NALM-master 1\GNLSE\._.DS_Store, 120 , 2019-03-05
Figure8_NALM-master 1\GNLSE\Solvers, 0 , 2016-06-08
Figure8_NALM-master 1\GNLSE\Solvers\IP_CQEM_FD.m, 4823 , 2016-06-08
Figure8_NALM-master 1\GNLSE\Solvers\IP_CQEM_TD.m, 4260 , 2016-06-08
Figure8_NALM-master 1\GNLSE\Solvers\Linearoperator_w.m, 409 , 2016-06-08
Figure8_NALM-master 1\GNLSE\Solvers\NonLinearoperator_w.m, 952 , 2016-06-08
Figure8_NALM-master 1\GNLSE\Solvers\Raman_response_w.m, 793 , 2016-06-08
Figure8_NALM-master 1\GNLSE\Solvers\SSFM_with_Raman.m, 3797 , 2016-06-08
Figure8_NALM-master 1\GNLSE\Solvers\UPM_SSFM.m, 3127 , 2016-06-08
Figure8_NALM-master 1\GNLSE\Solvers\UPM_SSFM_with_Raman.m, 3842 , 2016-06-08
Figure8_NALM-master 1\main.m, 4622 , 2016-06-08
Figure8_NALM-master 1\main2.m, 6407 , 2016-06-08
Figure8_NALM-master 1\main3.m, 7562 , 2016-06-08
Figure8_NALM-master 1\NonlinearEffects, 0 , 2016-06-08
Figure8_NALM-master 1\NonlinearEffects\main_PCF_DW.m, 3798 , 2016-06-08
Figure8_NALM-master 1\NonlinearEffects\main_SMF_N_order_Soliton.m, 4168 , 2016-06-08
Figure8_NALM-master 1\NonlinearEffects\main_SMF_RIFS.m, 3212 , 2016-06-08

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    说明：  利用LP01模式来对单模光纤模场直径与归一化频率的关系进行简单计算(Calculating the relationship between mode field diameter and normalized frequency of single mode fiber)
    2020-12-12 14:29:17下载
    积分：1
  • L1C
    余弦高斯光束图像，可以看到不同传输距离的光强，并且采用分数傅里叶讨论方法！(Cosine Gauss beam image)
    2017-09-11 17:58:27下载
    积分：1
  • Figure8_NALM-master 1
    NALM锁模激光器仿真，非线性环路反射镜锁模获得飞秒激光脉冲。(The simulation of NALM mode-locked laser shows that the femtosecond laser pulse can be obtained by mode-locked non-linear loop mirror.)
    2021-02-20 20:39:42下载
    积分：1
  • matlab
    利用LP01模式来对单模光纤模场直径与归一化频率的关系进行简单计算(Calculating the relationship between mode field diameter and normalized frequency of single mode fiber)
    2020-12-12 14:29:17下载
    积分：1
  • DFB_model
    利用numpy库实现激光器领域的时域行波模型。该模型输出激光器信号，频谱等。(The time-domain traveling wave model in laser field is realized by using numpy library. The model outputs laser signals, spectrum and so on.)
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  • LGintensity
    LG光束的光强和相位模拟，包括缔合拉盖尔多项式和相位屏(Intensity and Phase of LG Beams)
    2021-03-21 13:19:17下载
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    说明：  有效的解包裹程序：傅里叶变换相位解包裹程序(Fourier transform phase unwrapping program)
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  • 3
    说明：  涡旋光束的相息图。。。。。。。。。。。。(Simulated Chart of Vortex Beam)
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  • 有关涡旋光的产生和光栅生成的五个程序
    这五个程序是有关涡旋光的产生和光栅生成的程序。1.是单束涡旋光生成 2.生成叉形光栅。3.生成立体的涡旋光。4.生成不同拓扑荷数涡旋光对应相位图。5.生成正弦周期光栅和螺旋相位片图(These five programs are programs for the generation of vortex beams and the generation of grating. 1. is the generation of single beam of vortex light The 2. generation of fork shaped grating. 3. generation of three-dimensional vortex light. 4. the phase diagram of the different topological charge vortex optical rotation is generated. 5. generation of sinusoidal periodic gratings and spiral phase plate)
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