Difference between revisions of "2012AnnihCountrRateEstimate"
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(Created page with ' ==Commissioning Plans== Prior to a beam commissioning run, the detector system will be calibrated in the Tunnel using a Na-22 and Co-60 source. The annihilation counter will a…') |
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+ | =Rate Estimates= | ||
− | == | + | ==Previous experiment at the IAC== |
− | + | {| border="3" cellpadding="20" cellspacing="0" | |
+ | | [[File:052008PosProdApparatus.png| 400 px]] || [[File:052008PosProdSignal.png| 200 px]] || [[File:052008PosProdBackgrd.png| 200 px]] | ||
+ | |- | ||
+ | | IAC apparatus for positron production experiment || Counts observed when the dipole is tuned to direct positrons onto the Ta target || Counts from electrons on Ta target | ||
+ | |} | ||
− | =Rate | + | ;HpGe observed about 1 annihilation photon per 10 microCoulombs of electrons on the upstream Tungsten target |
+ | ;Ratio of annihilation photons observed when using positrons to electrons 120 to 10 | ||
+ | |||
+ | {| border="3" cellpadding="20" cellspacing="0" | ||
+ | | Condition || Grade Calculation | ||
+ | |- | ||
+ | | Electron Beam Energy || 10 MeV | ||
+ | |- | ||
+ | | Peak current || 40 mA | ||
+ | |- | ||
+ | | Pulse width || 100 ns | ||
+ | |- | ||
+ | | Rep Rate || 300 Hz | ||
+ | |- | ||
+ | Bend 2 Dipole | ||
+ | |||
+ | |||
+ | Spot size at 2nd Dipole D2 | ||
+ | |||
+ | Spot size at Phosphorous Target | ||
− | + | |} | |
==NaI rate Ratio of positron to electron beam== | ==NaI rate Ratio of positron to electron beam== | ||
Line 14: | Line 38: | ||
Assume a 2 mm thick Tungsten target that is 1" square | Assume a 2 mm thick Tungsten target that is 1" square | ||
− | The target is located at -80 < Z < -80.2 | + | The target is located at -80 < Z < -80.2 |
− | The NaI crystal is 2.32" or 56.49 mm in diameter | + | |
− | The NaI crystal is 8" from the target then the opening angle is atan(2.32/8/2) = 8.25 degrees | + | The NaI crystal is 2.32" or 56.49 mm in diameter |
+ | |||
+ | The NaI crystal is 8" from the target then the opening angle is atan(2.32/8/2) = 8.25 degrees | ||
+ | |||
+ | ====Solid Angle==== | ||
+ | |||
+ | <math>\Omega = \frac{\pi (2.34)^2}{(8)^2} = 0.27 strad</math> | ||
+ | |||
+ | ===Chromox target === | ||
+ | |||
+ | Chromox target is 0.011" thick = 0.279 mm | ||
+ | |||
+ | [[File:Chromox_datasheet_CERN.pdf]] | ||
+ | |||
+ | ====G4 Chromox description==== | ||
+ | <pre> | ||
+ | G4Element* Cr = | ||
+ | new G4Element("Chromium", "Cr",z=24., a= 51.9961*g/mole); | ||
+ | |||
+ | G4Element* Al = | ||
+ | new G4Element("Aluminum","Al", z=13., a= 26.98154*g/mole); | ||
+ | |||
+ | |||
+ | // | ||
+ | // typically the viewers are 99.5% Al_2 O_3 and 0.5% Cr_2 O_3 | ||
+ | // | ||
+ | // I will construct a material that is 99.5% made of 2 Al and 3 O Atoms/nuclei | ||
+ | // and 0.5% made of 2 Cr and 3 O Atoms/nuclei | ||
+ | // | ||
+ | // Al = 99.5 * 2/5 = 39.8 % | ||
+ | // O = 99.5 * 3/5 = 59.7 % | ||
+ | // O = 0.5 * 3/5 = 0.3 % | ||
+ | // Cr = 0.5 * 2/5 = 0.2% | ||
+ | // | ||
+ | // Jlab PePPo Chromox viewer is 0.011" thick = 0.279 mm | ||
+ | // | ||
+ | // | ||
+ | |||
+ | G4Material* ChroMox = new G4Material("ChroMox", density= 3.85*g/cm3, nel=3); | ||
+ | ChroMox->AddElement(Al, 30.8*perCent); | ||
+ | ChroMox->AddElement(O, 60*perCent); | ||
+ | ChroMox->AddElement(Cr, 0.2*perCent); | ||
+ | |||
+ | </pre> | ||
+ | |||
+ | ==Rates using GEANT4== | ||
+ | |||
+ | Assume 3 MeV electron and positron beam. | ||
+ | |||
+ | ===2 mm Thick Tungsten annihilation target=== | ||
+ | |||
+ | Integrating between 0.3 and 0.7 MeV (511 peak unclear) | ||
+ | |||
+ | :<math>\frac{\mbox{Positrons}}{\mbox{electron}} = \frac{6768}{1367} = \frac{5}{1}</math> | ||
+ | |||
+ | Integrating between 0.5 and 0.53 MeV | ||
+ | |||
+ | :<math>\frac{\mbox{Positrons}}{\mbox{electron}} = \frac{2685}{120} = \frac{22}{1}</math> | ||
+ | |||
+ | ;Experiment at IAC had <math>\frac{12}{1}</math> | ||
+ | |||
+ | [[Image:G4AnihCountrRates_02022012.png | 200px]] | ||
+ | |||
+ | ===Chromox=== | ||
+ | |||
+ | The photon rates predicted by GEANT4 when electrons and positrons interact with the ChroMox target and enter one of the NaI detectors having a solid angle of (0.27 strad) | ||
+ | |||
+ | |||
+ | Integrating between 0.5 and 0.53 MeV | ||
+ | |||
+ | :<math>\frac{\mbox{Positrons}}{\mbox{electron}} = \frac{1094}{8.4} = \frac{130}{1}</math> | ||
+ | |||
+ | |||
+ | |||
+ | [[Image:G4AnihCountrRates_01252012.png | 200px]] | ||
[[PePPO_2012Run]] | [[PePPO_2012Run]] |
Latest revision as of 17:43, 2 February 2012
Rate Estimates
Previous experiment at the IAC
IAC apparatus for positron production experiment | Counts observed when the dipole is tuned to direct positrons onto the Ta target | Counts from electrons on Ta target |
- HpGe observed about 1 annihilation photon per 10 microCoulombs of electrons on the upstream Tungsten target
- Ratio of annihilation photons observed when using positrons to electrons 120 to 10
Condition | Grade Calculation |
Electron Beam Energy | 10 MeV |
Peak current | 40 mA |
Pulse width | 100 ns |
Rep Rate | 300 Hz |
NaI rate Ratio of positron to electron beam
Assumed Geometry
Assume a 2 mm thick Tungsten target that is 1" square
The target is located at -80 < Z < -80.2
The NaI crystal is 2.32" or 56.49 mm in diameter
The NaI crystal is 8" from the target then the opening angle is atan(2.32/8/2) = 8.25 degrees
Solid Angle
Chromox target
Chromox target is 0.011" thick = 0.279 mm
File:Chromox datasheet CERN.pdf
G4 Chromox description
G4Element* Cr = new G4Element("Chromium", "Cr",z=24., a= 51.9961*g/mole); G4Element* Al = new G4Element("Aluminum","Al", z=13., a= 26.98154*g/mole); // // typically the viewers are 99.5% Al_2 O_3 and 0.5% Cr_2 O_3 // // I will construct a material that is 99.5% made of 2 Al and 3 O Atoms/nuclei // and 0.5% made of 2 Cr and 3 O Atoms/nuclei // // Al = 99.5 * 2/5 = 39.8 % // O = 99.5 * 3/5 = 59.7 % // O = 0.5 * 3/5 = 0.3 % // Cr = 0.5 * 2/5 = 0.2% // // Jlab PePPo Chromox viewer is 0.011" thick = 0.279 mm // // G4Material* ChroMox = new G4Material("ChroMox", density= 3.85*g/cm3, nel=3); ChroMox->AddElement(Al, 30.8*perCent); ChroMox->AddElement(O, 60*perCent); ChroMox->AddElement(Cr, 0.2*perCent);
Rates using GEANT4
Assume 3 MeV electron and positron beam.
2 mm Thick Tungsten annihilation target
Integrating between 0.3 and 0.7 MeV (511 peak unclear)
Integrating between 0.5 and 0.53 MeV
- Experiment at IAC had
Chromox
The photon rates predicted by GEANT4 when electrons and positrons interact with the ChroMox target and enter one of the NaI detectors having a solid angle of (0.27 strad)
Integrating between 0.5 and 0.53 MeV