Open AccessA high‐power, high‐repetition‐rate THz source for pump–probe experiments at Linac Coherent Light Source II
Author(s) -
Zhang Z.,
Fisher A. S.,
Hoffmann M. C.,
Jacobson B.,
Kirchmann P. S.,
Lee W.-S.,
Lindenberg A.,
Marinelli A.,
Nanni E.,
Schoenlein R.,
Qian M.,
Sasaki S.,
Xu J.,
Huang Z.
Publication year - 2020
Publication title -
journal of synchrotron radiation
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.172
H-Index - 99
ISSN - 1600-5775
DOI - 10.1107/s1600577520005147
Subject(s) - wiggler , physics , terahertz radiation , optics , linear particle accelerator , undulator , laser , radiation , microsecond , free electron laser , optoelectronics , electron , beam (structure) , cathode ray , nuclear physics
Experiments using a THz pump and an X‐ray probe at an X‐ray free‐electron laser (XFEL) facility like the Linac Coherent Light Source II (LCLS II) require frequency‐tunable (3 to 20 THz), narrow bandwidth (∼10%), carrier‐envelope‐phase‐stable THz pulses that produce high fields (>1 MV cm −1 ) at the repetition rate of the X‐rays and are well synchronized with them. In this paper, a two‐bunch scheme to generate THz radiation at LCLS II is studied: the first bunch produces THz radiation in an electromagnet wiggler immediately following the LCLS II undulator that produces X‐rays from the second bunch. The initial time delay between the two bunches is optimized to compensate for the path difference in THz transport. The two‐bunch beam dynamics, the THz wiggler and radiation are described, as well as the transport system bringing the THz pulses from the wiggler to the experimental hall.