scholarly journals 1 m long continuously-written fibre Bragg gratings for combined second- and third-order dispersion compensation

1997 ◽  
Vol 33 (22) ◽  
pp. 1891 ◽  
Author(s):  
M. Durkin ◽  
M. Ibsen ◽  
M.J. Cole ◽  
R.I. Laming
2017 ◽  
Vol 42 (4) ◽  
pp. 811 ◽  
Author(s):  
Henry Timmers ◽  
Yuki Kobayashi ◽  
Kristina F. Chang ◽  
Maurizio Reduzzi ◽  
Daniel M. Neumark ◽  
...  

1994 ◽  
Vol 19 (19) ◽  
pp. 1550 ◽  
Author(s):  
June-Koo Rhee ◽  
James A. Arns ◽  
Willis S. Colburn ◽  
Thomas S. Sosnowski ◽  
Theodore B. Norris

2014 ◽  
Vol 2 ◽  
Author(s):  
Qingwei Yang ◽  
Xinglong Xie ◽  
Jun Kang ◽  
Haidong Zhu ◽  
Ailin Guo ◽  
...  

Abstract The dispersion of a pair of prisms is analyzed by means of a ray-tracing method operating at other than tip-to-tip propagation of the prisms, taking into consideration the limited spectral bandwidth. The variations of the group delay dispersion and the third-order dispersion for a pair of prisms are calculated with respect to the incident position and the separation between the prisms. The pair of prisms can provide a wide range of independent and continuous third-order dispersion compensation. The effect of residual third-order dispersion on the pulse contrast ratio and pulse duration is also calculated. The residual third-order dispersion not only worsens the pulse contrast ratio, but also increases the pulse duration to the hundreds of femtosecond range for a tens of femtosecond pulse, even when the residual third-order dispersion is small. These phenomena are helpful in compensating for the residual high-order dispersion and in understanding its effect on pulse contrast ratios and pulse durations in ultrashort laser systems.


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