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RIS citation export for TUPME055: Room-temperature Burst-mode GHz and THz Pulse-train Photoinjector

TY - CONF
AU - Chao, F.H.
AU - Chen, C.H.
AU - Chou, P.J.
AU - Huang, K.Y.
AU - Huang, Y.-C.
AU - Wang, Y.C.
AU - Wu, M.H.
ED - Petit-Jean-Genaz, Christine
ED - Arduini, Gianluigi
ED - Michel, Peter
ED - Schaa, Volker RW
TI - Room-temperature Burst-mode GHz and THz Pulse-train Photoinjector
J2 - Proc. of IPAC2014, Dresden, Germany, June 15-20, 2014
C1 - Dresden, Germany
T2 - International Particle Accelerator Conference
T3 - 5
LA - english
AB - A photoinjector usually generates an electron pulse with few ps pulse duration repeating at 10-100 Hz. The low-pulse rate limits the data rate in a number of applications. Although high-repetition-rate operation is possible from a superconducting accelerator, the high cost and complexity of a superconducting system prevent it from being widely used. In this paper, we present our study toward a burst-mode GHz/THz pulse train photoinjector operating at room temperature. For the GHz operation mode, we self-develop a driver laser system, generating tens of laser pulses at 2.856 GHz in an adjustable 5-10 ns temporal envelope repeating at 10 Hz. Upon illuminating the photocathode with the driver laser, our S-band photoinjector (supported by Tsing Hua University, Beijing) is to generate a GHz electron pulse train with the same temporal structure as that of the driver laser pulses. For the THz operation mode, we illuminate the photocathode with two lasers, one being a typical UV gun-driver laser at 260 nm and the other being a mid-infrared laser at 100 THz. The UV laser induces photoemission and the infrared laser gates the emission current at 100 THz by virtue of the Schottky effect.
PB - JACoW
CP - Geneva, Switzerland
SP - 1492
EP - 1494
KW - electron
KW - laser
KW - cathode
KW - bunching
KW - acceleration
DA - 2014/07
PY - 2014
SN - 978-3-95450-132-8
DO - 10.18429/JACoW-IPAC2014-TUPME055
UR - http://jacow.org/ipac2014/papers/tupme055.pdf
ER -