Tunable narrowband terahertz emission from mastered laser-electron beam interaction

被引:78
作者
Bielawski, S. [1 ,2 ]
Evain, C. [2 ]
Hara, T. [1 ,6 ]
Hosaka, M. [3 ]
Katoh, M. [1 ,4 ]
Kimura, S. [1 ,4 ]
Mochihashi, A. [1 ,4 ]
Shimada, M. [1 ]
Szwaj, C. [2 ]
Takahashi, T. [5 ]
Takashima, Y. [3 ]
机构
[1] Natl Inst Nat Sci, Inst Mol Sci, UVSOR Facil, Okazaki, Aichi 4448585, Japan
[2] Univ Sci & Tech Lille Flandres Artois, FR CNRS 2416, CERLA,UMR CNRS 8523, Lab PhLAM, F-59655 Villeneuve Dascq, France
[3] Nagoya Univ, Grad Sch Engn, Nagoya, Aichi 4648603, Japan
[4] Grad Univ Adv Studies SOKENDAI, Sch Phys Sci, Okazaki, Aichi 4448585, Japan
[5] Kyoto Univ, Inst Res Reactor, Osaka 5900494, Japan
[6] RIKEN, SPring Ctr 8, Harima Inst, Sayo, Hyogo 6795148, Japan
基金
日本学术振兴会;
关键词
D O I
10.1038/nphys916
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
In the quest for sources of optical radiation in the terahertz domain, promising candidates are nonlinear optical processes occurring when an intense laser beam interacts with a material medium(1-5). Besides conventional media (such as crystals), relativistic electrons also show striking nonlinear collective behaviours, which can lead to powerful laser-induced coherent emission(6,7), revealing huge potentials of these devices as terahertz sources(8). However, up to now only broadband emissions were reported, and experimental control of their radiation properties, such as their spectra(9,10), remained an important challenge. Here, we demonstrate the possibility of mastering the coherent emission experimentally by producing tunable narrowband terahertz radiation. The interaction is made to occur between an electron beam and laser pulses possessing a longitudinal quasi-sinusoidal modulation, and the narrowband emission occurs in a region of quasi-uniform magnetic field. The process therefore strongly differs from classical synchrotron radiation experiments, where narrowband emission occurs inside a periodic magnetic field.
引用
收藏
页码:390 / 393
页数:4
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