Difference between revisions of "2019-02-01-LeadershipReports"
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** | ** | ||
'''Yuhong Zhang''' | '''Yuhong Zhang''' | ||
| − | + | - Previous two weeks (Dec 28-Jan 4) | |
| − | JSPEC code development | + | - JSPEC code development |
| − | + | - RF Voltage calculation module has been finished and tested. This feature has been merged into the main branch | |
| − | + | and pushed to Github. When the bunch size is chosen to be constant, jspec will calculate the RF voltage with | |
| − | + | respect to the momentum spread at each time step. The voltage is saved in the last row of the user-specified | |
| − | + | output file. When the bunch size is allowed to vary with the momentum spread. The RF voltage is calculated once. | |
| − | + | But it is still saved as above on each time step. | |
| − | + | - Space charge field of the electron bunch results in both the longitudinal velocity shift and the transverse velocity | |
| − | + | shift of the electrons. The longitudinal velocity shift is due to the electrostatic potential difference according to | |
| − | + | the different radius. The transverse one is due to the collective effect of the radial space charge field and the | |
| − | + | longitudinal magnetic field. In the perspective of the friction force calculation, both velocity shifts change the | |
| − | + | relative velocity between the ion and the electron while the transverse one also changes the electron temperature (Larmor | |
| − | + | emittance). With the help of some references, the formulas of the velocity drift for a uniform round electron beam | |
| − | + | (bunched or coasting) are derived and documented. These are good enough for IMP experiment. For a uniform flat beam, | |
| − | + | one may have to do numerical integration. The code is still under development. | |
| − | + | - For the core-tail model, I am working on the multidimensional fitting algorithm using the gradient descent method. | |
| − | + | - Next two weeks (Jan 7 - Jan 11) | |
** | ** | ||
Revision as of 10:05, 23 May 2019
Accelerator Physics - T. Satogata (CASA Director)
Todd Satogata
- Previous two weeks (Dec 28 - Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Alex Bogacz
- Previous two weeks (Dec 28 - Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Rui Li
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Edy Nissen
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Chris Tennant
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Accelerator R & D - Y. Zhang
Fanglei Lin
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Vasiliy Morozov
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Amy Sy
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Yuhong Zhang
- Previous two weeks (Dec 28-Jan 4)
- JSPEC code development
- RF Voltage calculation module has been finished and tested. This feature has been merged into the main branch
and pushed to Github. When the bunch size is chosen to be constant, jspec will calculate the RF voltage with
respect to the momentum spread at each time step. The voltage is saved in the last row of the user-specified
output file. When the bunch size is allowed to vary with the momentum spread. The RF voltage is calculated once.
But it is still saved as above on each time step.
- Space charge field of the electron bunch results in both the longitudinal velocity shift and the transverse velocity
shift of the electrons. The longitudinal velocity shift is due to the electrostatic potential difference according to
the different radius. The transverse one is due to the collective effect of the radial space charge field and the
longitudinal magnetic field. In the perspective of the friction force calculation, both velocity shifts change the
relative velocity between the ion and the electron while the transverse one also changes the electron temperature (Larmor
emittance). With the help of some references, the formulas of the velocity drift for a uniform round electron beam
(bunched or coasting) are derived and documented. These are good enough for IMP experiment. For a uniform flat beam,
one may have to do numerical integration. The code is still under development.
- For the core-tail model, I am working on the multidimensional fitting algorithm using the gradient descent method.
- Next two weeks (Jan 7 - Jan 11)
Computational Physics - Y. Roblin
Yves Roblin
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
He Zhang
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Kirsten Deitrick
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Diagnostic Development - K. Jordan
Kevin Jordan
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Joe Gubeli
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
Michael Tiefenback
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
LERF - S. Benson
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)
A. Hutton
- Previous two weeks (Dec 28-Jan 4)
- Next two weeks (Jan 7 - Jan 11)