Independent and continuous third-order dispersion compensation using a pair of prisms

Qingwei Yang; Xinglong Xie; Jun Kang; Haidong Zhu; Ailin Guo; and Qi Gao

doi:10.1017/hpl.2014.40

Journals >High Power Laser Science and Engineering >Volume 2 >Issue 4 >Page 04000e38 > Article

High Power Laser Science and Engineering
Vol. 2, Issue 4, 04000e38 (2014)

Independent and continuous third-order dispersion compensation using a pair of prisms

Qingwei Yang^*, Xinglong Xie, Jun Kang, Haidong Zhu, Ailin Guo, and and Qi Gao

Author Affiliations

National Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, No. 390, Qinghe Road, Jiading District, Shanghai 201800, China

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DOI: 10.1017/hpl.2014.40 Cite this Article Set citation alerts

Qingwei Yang, Xinglong Xie, Jun Kang, Haidong Zhu, Ailin Guo, and Qi Gao. Independent and continuous third-order dispersion compensation using a pair of prisms[J]. High Power Laser Science and Engineering, 2014, 2(4): 04000e38 Copy Citation Text

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Fig. 1. Ray-tracing sketch for a pair of identical isosceles prisms in a parallel face configuration.

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At the central wavelength, GDD and TOD change with . Material: ; simulation parameters: , , , , , and .

Fig. 2. At the central wavelength, GDD and TOD change with

. Material:

; simulation parameters:

, and

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Fig. 3. At the central wavelength, GDD and TOD change with

. Material:

; simulation parameters:

, and

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Fig. 4. At the central wavelength, GDD and TOD change with

. Material:

; simulation parameters:

, and

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Fig. 5. At the central wavelength, TOD changes with

and

when

. Simulation parameters:

, and

; material:

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Fig. 6. At the central wavelength, TOD changes with

and

when

. Simulation parameters:

, and

; material: SF10.

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Fig. 7. Effect of RTOD on the pulse contrast ratio. (b) is a magnified section of (a).

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Fig. 8. Effect of RTOD on pulse duration. The figure on the right is a magnified section of the figure on the left.

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Material	$B_{1}$	$B_{2}$	$B_{3}$	$C_{1}$	$C_{2}$	$C_{3}$
	5.67588800E001	4.71091400E001	3.84847230E000	2.52643000E003	1.00783330E002	1.20055600E003
SF10	1.61625977E000	2.59229334E001	1.07762317E000	1.27534559E002	5.81983954E002	1.16607680E002