Difference between revisions of "Mar 27, 2020 Meeting Minutes"
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− | + | ==Emails/attachments sent during the previous week== | |
+ | *None | ||
+ | |||
+ | ==Post-meeting notes== | ||
+ | *Currently implementing GPT Maxwellian distribution generator C++ code from Cristhian - ion energies will be derived from this distribution | ||
+ | *Cristian presented results of ions moving within the electron beam potential. Up to z=0.65m, ions move towards the photocathode on average | ||
+ | *Create simulation using pulses of electrons of 50ps with 2ns spacing | ||
+ | *What is the outgassing rate when ions hit the beampipe? | ||
+ | *What is the charge neutralization time (i.e. when N_ions=N_electrons)? | ||
+ | *Josh can present the "ion trap" simulations using FEMM model with steel shield. | ||
[[Ionization Effects Meetings | Return to Ionization Effects Meetings]] | [[Ionization Effects Meetings | Return to Ionization Effects Meetings]] | ||
[[Weekly phone call - Mar 27, 2020 | Go to Meeting Page]] | [[Weekly phone call - Mar 27, 2020 | Go to Meeting Page]] |
Latest revision as of 09:19, 2 April 2020
Emails/attachments sent during the previous week
- None
Post-meeting notes
- Currently implementing GPT Maxwellian distribution generator C++ code from Cristhian - ion energies will be derived from this distribution
- Cristian presented results of ions moving within the electron beam potential. Up to z=0.65m, ions move towards the photocathode on average
- Create simulation using pulses of electrons of 50ps with 2ns spacing
- What is the outgassing rate when ions hit the beampipe?
- What is the charge neutralization time (i.e. when N_ions=N_electrons)?
- Josh can present the "ion trap" simulations using FEMM model with steel shield.