A simulation of coherent and super-radiant Smith-Purcell radiation is performed in the gigahertz regime using a three-dimensional particle-in-cell code. The simulation model supposes a rectangular grating to be driven by a single electron bunch and a train of periodic bunches, respectively. The true Smith-Purcell radiation is distinguished from the evanescent wave, which has an angle independent frequency lower than the minimum allowed Smith-Purcell frequency. We also find that the super-radiant radiations excited by periodic bunches are emitted at higher harmonics of the bunching frequency and at the corresponding Smith-Purcell angles.
REFERENCES
1.
J.
Urata
, M.
Goldstein
, M. F.
Kimmitt
, A.
Naumov
, C.
Platt
, and J. E.
Walsh
, Phys. Rev. Lett.
80
, 516
(1998
).2.
A.
Bakhtyari
, J. E.
Walsh
, and J. H.
Brownell
, Phys. Rev. E
65
, 066503
(2002
).3.
4.
L.
Schachter
and A.
Ron
, Phys. Rev. A
40
, 876
(1989
).5.
K.-J.
Kim
and S.-B.
Song
, Nucl. Instrum. Methods Phys. Res. A
475
, 158
(2001
).6.
H. L.
Andrews
and C. A.
Brau
, Phys. Rev. ST Accel. Beams
7
, 070701
(2004
).7.
H. L.
Andrews
, C. H.
Boulware
, C. A.
Brau
, and J. D.
Jarvis
, Phys. Rev. ST Accel. Beams
8
, 050703
(2005
).8.
V.
Kumar
and K.-J.
Kim
, Phys. Rev. E
73
, 026501
(2006
).9.
L.
Ludeking
, the MAGIC user’s manual.10.
D.
Li
, Z.
Yang
, K.
Imasaki
, and Gun-sik
Park
, Phys. Rev. ST Accel. Beams
9
, 040701
(2006
).11.
H. L.
Andrews
, C. H.
Boulware
, C. A.
Brau
, and J. D.
Jarvis
, Phys. Rev. ST Accel. Beams
8
, 110720
(2005
).12.
S. E.
Korbly
, A. S.
Kesar
, J. R.
Sirigiri
, and R. J.
Temkin
, Phys. Rev. Lett.
94
, 054803
(2005
).13.
J. T.
Donohue
and J.
Gardelle
, Phys. Rev. ST Accel. Beams
8
, 060702
(2005
).© 2006 American Institute of Physics.
2006
American Institute of Physics
You do not currently have access to this content.