High Power Laser Science and Engineering, 2014, 2 (4): 04000e38, Published Online: Jan. 13, 2015
Independent and continuous third-order dispersion compensation using a pair of prisms 
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Figures & Tables
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.
Table1. Sellmeier coefficients for Equation (7 ) obtained from the Thorlab catalog[17].
|
001
001
000
003
002
003
000
001
000
002
002
002Qingwei Yang, Xinglong Xie, Jun Kang, Haidong Zhu, Ailin Guo, 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.
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