Second Harmonic Generation in CdTe Plate by Free Electron Laser

2000 ◽  
Vol 39 (Part 1, No. 10) ◽  
pp. 5912-5913
Author(s):  
Toshihiko Yamauchi ◽  
Nobuhiro Kikuzawa ◽  
Eisuke Minehara ◽  
Ryoji Nagai ◽  
Nobuyuki Nishimori ◽  
...  
2002 ◽  
Vol 41 (Part 1, No. 11A) ◽  
pp. 6360-6363 ◽  
Author(s):  
Toshihiko Yamauchi ◽  
Nobuhiro Kikuzawa ◽  
Eisuke Minehara

2018 ◽  
Vol 120 (22) ◽  
Author(s):  
Sh. Yamamoto ◽  
T. Omi ◽  
H. Akai ◽  
Y. Kubota ◽  
Y. Takahashi ◽  
...  

2015 ◽  
Vol 107 (8) ◽  
pp. 081101 ◽  
Author(s):  
Alexander Paarmann ◽  
Ilya Razdolski ◽  
Alexey Melnikov ◽  
Sandy Gewinner ◽  
Wieland Schöllkopf ◽  
...  

2021 ◽  
Vol 28 (3) ◽  
Author(s):  
A. M. Kalitenko

A numerical study of the effect of betatron oscillations on the second harmonic generation in free-electron lasers (FELs) is presented. Analytical expressions for the effective coupling strength factors are derived that clearly distinguish all contributions in subharmonics and each polarization of the radiation. A three-dimensional time-dependent numerical FEL code that takes into account the main FEL effects and the individual contribution of each electron to the second harmonic generation is presented. Also, the X- and Y-polarizations of the second harmonic are analyzed. The second harmonic was detected in experiments at the Advanced Photon Source (APS) Low Energy Undulator Test Line (LEUTL) and Linac Coherent Light Source (LCLS) in the soft X-ray regime. The approach presented in the article can be useful for a comprehensive study and diagnostics of XFELs. In the paper, the LCLS and Pohang Accelerator Laboratory X-ray Free-Electron Laser (PAL-XFEL) experiments are modeled. The simulation results are in a good agreement with the experimental data.


1986 ◽  
Vol 83 ◽  
Author(s):  
K. J. Song ◽  
D. Heskett ◽  
L. Urbach ◽  
H. L. Dai ◽  
E. W. Plummer

ABSTRACTThe sensitivity of second harmonic generation at interfaces has been utilized to probe the spatial and frequency dependence of the local field generated near the surface of a nearly free electron metal by an externally imposed electromagnetic field. The longitudinal screening field was found to oscillate with a wavelength on the order of 10Å and to propagate into the bulk several layers deep.


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