Learn about Mu2e-II: Difference between revisions
Jump to navigation
Jump to search
No edit summary |
No edit summary |
||
Line 33: | Line 33: | ||
|- | |- | ||
| Peak bunch size || 2<math>\small{\times 10^8}</math> || (5 mA, can't be changed quickly) | | Peak bunch size || 2<math>\small{\times 10^8}</math> || (5 mA, can't be changed quickly) | ||
| | |||
| Bunch size to Mu2e-II || 1.4<math>\small{\times 10^8}</math> || (for 2 mA average current) | |||
|- | |- | ||
| RF frequency || 162.5 || MHz, full bunch rate from PIP-II | | RF frequency || 162.5 || MHz, full bunch rate from PIP-II |
Revision as of 22:03, 29 September 2021
Parameter | Nominal value | Units, Comments | ||||
---|---|---|---|---|---|---|
PIP-II parameters | ||||||
Beam energy (kinetic) | 800 | MeV | ||||
1.28[math]\displaystyle{ \small{\times 10^{-10}} }[/math] | J | |||||
I_average | 2 | mA (5 mA peak) | ||||
Bunch length | 4 | ps ([math]\displaystyle{ \sigma_t }[/math]) | ||||
[math]\displaystyle{ \epsilon_L }[/math] | 1.1 | ns-keV (rms) | ||||
[math]\displaystyle{ \sigma_E }[/math] | 275 | keV ([math]\displaystyle{ \epsilon_L/\sigma_t }[/math]) | ||||
PIP-II booster pulse | ||||||
Particles/pulse | 6.7[math]\displaystyle{ \small{\times 10^{12}} }[/math] | |||||
Pulse length | 550 | [math]\displaystyle{ \small\mu }[/math]s | ||||
Pulse rep rate | 20 | Hz | ||||
Bunch pattern | programmable | |||||
Bunch size | 0.8[math]\displaystyle{ \small{\times 10^8} }[/math] | (2 mA, CW) | ||||
Peak bunch size | 2[math]\displaystyle{ \small{\times 10^8} }[/math] | (5 mA, can't be changed quickly) | Bunch size to Mu2e-II | 1.4[math]\displaystyle{ \small{\times 10^8} }[/math] | (for 2 mA average current) | |
RF frequency | 162.5 | MHz, full bunch rate from PIP-II | ||||
325 | MHz | |||||
650 | MHz | |||||
Operation | 40 | wk/yr | ||||
Up time in operation | 90 | % | ||||
Mu2e-II parameters | ||||||
Bunch frequency | 81.25 | MHz (assumes 1/2 of 162.5 available) | ||||
Calibration, background, special runs | 30 | % | ||||
CE data | 70 | % | ||||
Mu2e-II efficiency | 100 | % | ||||
CE run time/yr | 1.5[math]\displaystyle{ \small{\times 10^{7}} }[/math] | s | ||||
Duration of run | 4 | yr | ||||
Total run time | 6[math]\displaystyle{ \small{\times 10^7} }[/math] | s | ||||
Total linac reps | 1.2[math]\displaystyle{ \small{\times 10^{9}} }[/math] | |||||
Extinction | 1[math]\displaystyle{ \small{\times 10^{-11}} }[/math] | [1[math]\displaystyle{ \small{\times 10^{-13}} }[/math] for 100x safety margin] | ||||
Beam power | 120 | kW (100 kW nominal) | ||||
Number of bunches/spill | 8 | (at 81.25 MHz) | ||||
Spill width | 100 | ns | ||||
Production target parameters | ||||||
Material | ||||||
Power deposition | kW | |||||
Optimizable parameters for stopping target material | ||||||
Aluminum stopping target | ||||||
Spill period | 1693 | ns | ||||
Spills/linac rep | 27770 | approximate, at 20 Hz linac repetition rate | ||||
Protons/spill | 1.6[math]\displaystyle{ \small{\times 10^{9}} }[/math] | (5 mA) | ||||
POT | 5[math]\displaystyle{ \small{\times 10^{22}} }[/math] | |||||
Stopped mu/p | 1.9[math]\displaystyle{ \small{\times 10^{-4}} }[/math] | rough estimate, TBC, assumes stopped mu/kW same at 800 and 8000 MeV among possibly other things | ||||
SES | <3[math]\displaystyle{ \small{\times 10^{-18}} }[/math] | |||||
E(conversion e-) | 104.97 | MeV | ||||
tau(muon) | 864 | ns | ||||
Lead stopping target | ||||||
E(conversion e-) | 94.9 | MeV | ||||
Tracker | ||||||
Resolution at 100 MeV | ||||||
Calorimeter | ||||||
Material | ||||||
Energy resolution | 5% | % (FWHM/2.36) | ||||
Time resolution | < 500 | ps | ||||
Position resolution | 10 | mm | ||||
Radiation dose | 10 | kGy/yr | ||||
[math]\displaystyle{ \small 1\times 10^{13} }[/math] | n/cm[math]\displaystyle{ \small{^2} }[/math] (total 1 MeV equivalent) | |||||
Cosmic Ray Veto | ||||||
Trigger/DAQ | ||||||
Event size | 1 | MB | ||||
Tape storage | 14 | PB/yr |