Collection Of theses on high power laser and plasma physics, 2013, 11 (1): 0029, Published Online: Jun. 2, 2017  

Beam positioning stability analysis on large laser facilities

Author Affiliations
Key Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences,Shanghai 201800, China
Figures & Tables

Fig. 1. Schematic of a single laser beam in a laser-driven ICF facility without mirrors.

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Fig. 2. Schematic diagram of a mirror in spatial filter ).

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Fig. 3. Variance of weighing factors in laser-driven ICF facilities.

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Fig. 4. SFLVWFs comparison of the SG-II facilities.

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Fig. 5. SFMVWF comparison of SG-II facilities.

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Fig. 6. SFLVWF comparison in different FPA systems.

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Fig. 7. SFMVWF comparison in different FPA systems.

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Fig. 8. Modules isolated from the other modules.

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Fig. 9. Steel trusses filled with concrete that decreased the responses around modal frequencies.

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Fig. 10. Beams bounded together preventing error accumulation.

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Table1. Optical parameters of SG-II Origin.

Spatial filters${f}_{i, 2} ~(\mathrm{m} )$${m}_{i} $${q}_{i} $${p}_{i} $
${\mathrm{SF} }_{0} $1.02.0000.00340.0034
${\mathrm{SF} }_{1} $1.95592.4550.00430.0069
${\mathrm{SF} }_{2} $1.86003.0140.01370.0169
${\mathrm{SF} }_{3} $4.63.4330.01900.0503
${\mathrm{SF} }_{4} $1.75210.04990.1749
${\mathrm{SF} }_{5} $3.951.8190.04030.1749
${\mathrm{SF} }_{6} $3.2311.4300.07040.3181
${\mathrm{SF} }_{7} $9.8562.2430.05180.4549
${\mathrm{SF} }_{8} $14.5021.4700.05171.0204
Focusing lens${f}_{T} = 0. 75$${q}_{T} = 1$${p}_{T} = 1. 5$

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Table2. Optical parameters of SG-II Additional beam.

Spatial filters${f}_{i, 2} ~(\mathrm{m} )$${m}_{i} $${q}_{i} $${p}_{i} $
${\mathrm{SF} }_{0} $1.02.0000.00610.0061
${\mathrm{SF} }_{1} $1.95592.4550.00760.0121
${\mathrm{SF} }_{2} $1.86003.0140.02410.0297
${\mathrm{SF} }_{3} $2.38252.9600.05560.0896
${\mathrm{SF} }_{4} $1.99712.0000.13270.2651
${\mathrm{SF} }_{5} $4.08081.5000.09740.5302
${\mathrm{SF} }_{6} $4.86432.1200.17330.7953
${\mathrm{SF} }_{7} $5.65471.7300.25791.6859
${\mathrm{SF} }_{8} $8.48761.0800.18562.9167
Focusing lens${f}_{T} = 1. 575$${q}_{T} = 1$${p}_{T} = 3. 1500$

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Table3. Optical parameters of SG-II Updated.

Spatial filters${f}_{i, 2} ~(\mathrm{m} )$${m}_{i} $${q}_{i} $${p}_{i} $
${\mathrm{SF} }_{0} $1.80010.04000.1441
${\mathrm{SF} }_{1} $2.0801.60.05540.1441
${\mathrm{SF} }_{2} $2.8501.50.06070.2306
${\mathrm{SF} }_{3} $2.60020.13300.3459
${\mathrm{SF} }_{4} $16.0006.45840.13960.6918
${\mathrm{SF} }_{5} $11.1170.93550.18804.4680
${\mathrm{SF} }_{6} $11.8831.06890.18804.1800
${\mathrm{SF} }_{7} $11.1170.93550.18804.4680
${\mathrm{SF} }_{8} $11.8831.06890.18804.1800
${\mathrm{SF} }_{9} $16.00010.13964.4680
Focusing lens${f}_{T} = 2. 234$${q}_{T} = 1$${p}_{T} = 4. 468$

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Table4. Experimental parameters in a four-pass amplification system.

Lenses in four-pass amplification (FPA)CSF-L1 (m)CSF-L2 (m)Beam aperture magnification ratio
Real parameters in SG-II updated11.88311.1170.9355
First fictional parameters20100.5
Second fictional parameters1050.5

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Fang Liu, Zhigang Liu, Liunian Zheng, Hongbiao Huang, Jianqiang Zhu. Beam positioning stability analysis on large laser facilities[J]. Collection Of theses on high power laser and plasma physics, 2013, 11(1): 0029.

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