High Power Laser Science and Engineering, Volume. 2, Issue 4, 04000e38(2014)
Independent and continuous third-order dispersion compensation using a pair of prisms
Figures & Tables(9)
Fig. 1. Ray-tracing sketch for a pair of identical isosceles prisms in a parallel face configuration.
Fig. 2. At the central wavelength, GDD and TOD change with 
. Material: 
; simulation parameters: 
, 
, 
, 
, 
, and 
.
Fig. 3. At the central wavelength, GDD and TOD change with 
. Material: 
; simulation parameters: 
, 
, 
, 
, 
, and 
.
Fig. 4. At the central wavelength, GDD and TOD change with 
. Material: 
; simulation parameters: 
, 
, 
, 
, 
, and 
.
Fig. 5. At the central wavelength, TOD changes with 
and 
when 
. Simulation parameters: 
, 
, 
, 
, and 
; material: 
.
Fig. 6. At the central wavelength, TOD changes with 
and 
when 
. Simulation parameters: 
, 
, 
, 
, and 
; material: SF10.
Fig. 7. Effect of RTOD on the pulse contrast ratio. (b) is a magnified section of (a).
Fig. 8. Effect of RTOD on pulse duration. The figure on the right is a magnified section of the figure on the left.
Table 1. Sellmeier coefficients for Equation (
7 ) obtained from the Thorlab catalog[17].View tableView in ArticleTable 1. Sellmeier coefficients for Equation (
7 ) obtained from the Thorlab catalog[17].Material $B_{1}$ $B_{2}$ $B_{3}$ $C_{1}$ $C_{2}$ $C_{3}$ 
5.67588800E 
0014.71091400E 
0013.84847230E 
0002.52643000E 
0031.00783330E 
0021.20055600E 
003SF10 1.61625977E 
0002.59229334E 
0011.07762317E 
0001.27534559E 
0025.81983954E 
0021.16607680E 
002
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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
Paper Information
Category: regular articles
Received: Feb. 15, 2014
Accepted: Apr. 11, 2014
Published Online: Jan. 13, 2015
The Author Email: Qingwei Yang (yqwphy@siom.ac.cn)
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