Abstract
Low emittance sub-picosecond electron pulses are expected to be used in a wide field, such as free electron laser, laser acceleration, femtosecond X-ray generation by inverse Compton scattering, and pulse radiolysis, etc. In order to produce the low emittance sub-picosecond electron pulses, we are developing a compact racetrack microtron (RTM) with a new 5 MeV injection system adopting an laser photo cathode RF gun. The operation of RTM is kept under the steady state of beam loading for long pulse mode so far. We have investigated for the first time by numerical simulation in the case of short- and single-pulse acceleration. As the results, RTM is also useful to accelerate a picosecond electron pulse under a transient state of beam loading. In the simulation, a picosecond electron pulse is accelerated to 139 MeV in RTM for the injection of about 5 MeV pulse with pulse length of 3 picoseconds, charge of 1 nC per pulse, and emittance of 1.8 πmm mrad, which corresponds of output of the RF gun.
| Original language | English |
|---|---|
| Title of host publication | Proceedings of the IEEE Particle Accelerator Conference |
| Place of Publication | Piscataway, NJ, United States |
| Publisher | IEEE |
| Pages | 2298-2300 |
| Number of pages | 3 |
| Volume | 4 |
| Publication status | Published - 1999 |
| Event | The 18th Biennial Particle Accelerator Conference - New York, NY, USA Duration: 1999 Mar 27 → 1999 Apr 2 |
Other
| Other | The 18th Biennial Particle Accelerator Conference |
|---|---|
| City | New York, NY, USA |
| Period | 99/3/27 → 99/4/2 |
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ASJC Scopus subject areas
- Engineering(all)
Cite this
Simulations of racetrack microtron for acceleration of picosecond electron pulse. / Washio, Masakazu; Kuroda, R.; Yang, J.; Hori, T.; Sakai, F.
Proceedings of the IEEE Particle Accelerator Conference. Vol. 4 Piscataway, NJ, United States : IEEE, 1999. p. 2298-2300.Research output: Chapter in Book/Report/Conference proceeding › Conference contribution
}
TY - GEN
T1 - Simulations of racetrack microtron for acceleration of picosecond electron pulse
AU - Washio, Masakazu
AU - Kuroda, R.
AU - Yang, J.
AU - Hori, T.
AU - Sakai, F.
PY - 1999
Y1 - 1999
N2 - Low emittance sub-picosecond electron pulses are expected to be used in a wide field, such as free electron laser, laser acceleration, femtosecond X-ray generation by inverse Compton scattering, and pulse radiolysis, etc. In order to produce the low emittance sub-picosecond electron pulses, we are developing a compact racetrack microtron (RTM) with a new 5 MeV injection system adopting an laser photo cathode RF gun. The operation of RTM is kept under the steady state of beam loading for long pulse mode so far. We have investigated for the first time by numerical simulation in the case of short- and single-pulse acceleration. As the results, RTM is also useful to accelerate a picosecond electron pulse under a transient state of beam loading. In the simulation, a picosecond electron pulse is accelerated to 139 MeV in RTM for the injection of about 5 MeV pulse with pulse length of 3 picoseconds, charge of 1 nC per pulse, and emittance of 1.8 πmm mrad, which corresponds of output of the RF gun.
AB - Low emittance sub-picosecond electron pulses are expected to be used in a wide field, such as free electron laser, laser acceleration, femtosecond X-ray generation by inverse Compton scattering, and pulse radiolysis, etc. In order to produce the low emittance sub-picosecond electron pulses, we are developing a compact racetrack microtron (RTM) with a new 5 MeV injection system adopting an laser photo cathode RF gun. The operation of RTM is kept under the steady state of beam loading for long pulse mode so far. We have investigated for the first time by numerical simulation in the case of short- and single-pulse acceleration. As the results, RTM is also useful to accelerate a picosecond electron pulse under a transient state of beam loading. In the simulation, a picosecond electron pulse is accelerated to 139 MeV in RTM for the injection of about 5 MeV pulse with pulse length of 3 picoseconds, charge of 1 nC per pulse, and emittance of 1.8 πmm mrad, which corresponds of output of the RF gun.
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M3 - Conference contribution
AN - SCOPUS:0033345496
VL - 4
SP - 2298
EP - 2300
BT - Proceedings of the IEEE Particle Accelerator Conference
PB - IEEE
CY - Piscataway, NJ, United States
ER -