Difference between revisions of "PAA ResultsFromTheIAC"
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| + | ==Nickel Normaization== | ||
| + | [[Ni-08-22-13]] | ||
| − | =Scotch Tape -vs- Kapton tape== | + | == Flux Rates on Jack== |
| + | |||
| + | ===Jack Photon Flux=== | ||
| + | |||
| + | [[JackPhotonFlux_06-04-2018]] | ||
| + | |||
| + | ===Jack Neutron Flux=== | ||
| + | |||
| + | [[NAA_SolarPanel]] | ||
| + | |||
| + | ==Scotch Tape -vs- Kapton tape== | ||
A 20 MeV electron was used to make a bremsstrahlung beam that impinged a sample of regular Scotch Tape and Kapton tape. Both tapes had similar areas of 2.5 x 3 cm. The Kapton had twice as much mass as the Scotch (0.1247 g -vs 0.0699 g). | A 20 MeV electron was used to make a bremsstrahlung beam that impinged a sample of regular Scotch Tape and Kapton tape. Both tapes had similar areas of 2.5 x 3 cm. The Kapton had twice as much mass as the Scotch (0.1247 g -vs 0.0699 g). | ||
| Line 7: | Line 19: | ||
The scotch taper became brittle after 4 hours of irradiation on the 25 N machine. | The scotch taper became brittle after 4 hours of irradiation on the 25 N machine. | ||
| − | Below is an uncalibrated spectrum using Thorium rods. Lines should appear at 2614 and | + | Below is an uncalibrated spectrum using Thorium rods. Lines should appear at 238.8,338.8, 511, 583.4, 911.2, and 2614.6 keV |
| + | |||
| + | |||
| + | |||
| + | {| border="3" cellpadding="5" cellspacing="0" | ||
| + | | Channel|| Energy (keV) | ||
| + | |- | ||
| + | |242 || 238.8 | ||
| + | |- | ||
| + | |342 || 338.8 | ||
| + | |- | ||
| + | |514 || 511 | ||
| + | |- | ||
| + | |586 || 583 | ||
| + | |- | ||
| + | |914 || 911.2 | ||
| + | |- | ||
| + | |2617 || 2614.6 | ||
| + | |} | ||
| + | |||
| + | slope=1.0003 +/- 0.000156023 | ||
| + | y-intercept=-3.12645 +/- 0.185346 | ||
| + | |||
| + | MPA->Draw("-3.12645+1.0003*evt.Chan>>(8000,0,8000)"); | ||
| + | |||
| + | Scotch tape run was 6663.4 seconds long (MPA->Draw("-3.12645+1.0003*evt.Chan>>NScotchTape(8000,0,8000)","0.00015");) | ||
| + | |||
| + | Kapton Tape run was 488.44 seconds long (MPA->Draw("-3.12645+1.0003*evt.Chan>>NKaptonTape(8000,0,8000)","0.0020473344");) | ||
| + | |||
| + | |||
| + | |||
| + | [[File:IrradiatedKapton-vsScotchTapeRates_9-22-16.png | 400 px]] | ||
| + | |||
| + | ==HEU disks== | ||
| + | |||
| + | A 20 MeV electron was used to make a bremsstrahlung beam that impinged HEU disks | ||
| + | |||
| + | |||
| + | Below is an uncalibrated spectrum using Thorium rods on Detector D. Lines should appear at 238.8,338.8, 511, 583.4, 911.2, and 2614.6 keV | ||
| + | |||
| + | The HEU samples were measured on two different HpGe detectors that has similar efficiencies. Get B was used for the Unirradiate sample and Detector D for the Irradiated HEU disk. | ||
| + | |||
| + | |||
| + | === Det D calibrations=== | ||
| + | {| border="3" cellpadding="5" cellspacing="0" | ||
| + | | Channel|| Energy (keV) | ||
| + | |- | ||
| + | |236 || 238.8 | ||
| + | |- | ||
| + | |334 || 338.8 | ||
| + | |- | ||
| + | |505 || 511 | ||
| + | |- | ||
| + | |576 || 583 | ||
| + | |- | ||
| + | |901 || 911.2 | ||
| + | |- | ||
| + | |2586 || 2614.6 | ||
| + | |} | ||
| + | |||
| + | slope=1.0108 +/- 0.000328475 | ||
| + | y-intercept=0.6533 +/- 0.385247 | ||
| + | |||
| + | MPA->Draw("0.6533+1.0108*evt.Chan>>(8000,0,8000)"); | ||
| + | |||
| + | |||
| + | ===HEU comparison Before and After irradiation=== | ||
| + | |||
| + | Uniradiated HEU sample was measured for 2671.8 seconds | ||
| + | |||
| + | MPA->Draw("-3.12645+1.0003*evt.Chan>>NHEUback(2000,0,8000)","0.0003742795"); | ||
| + | Iradiated HEU sample was measured overnight for 50554.469 seconds (14 hours) | ||
| + | MPA->Draw("0.6533+1.0108*evt.Chan>>NIradHEU(2000,0,8000)","0.00001978064"); | ||
[[PAA_Research]] | [[PAA_Research]] | ||
Latest revision as of 23:09, 14 June 2018
Nickel Normaization
Flux Rates on Jack
Jack Photon Flux
Jack Neutron Flux
Scotch Tape -vs- Kapton tape
A 20 MeV electron was used to make a bremsstrahlung beam that impinged a sample of regular Scotch Tape and Kapton tape. Both tapes had similar areas of 2.5 x 3 cm. The Kapton had twice as much mass as the Scotch (0.1247 g -vs 0.0699 g).
The scotch taper became brittle after 4 hours of irradiation on the 25 N machine.
Below is an uncalibrated spectrum using Thorium rods. Lines should appear at 238.8,338.8, 511, 583.4, 911.2, and 2614.6 keV
| Channel | Energy (keV) |
| 242 | 238.8 |
| 342 | 338.8 |
| 514 | 511 |
| 586 | 583 |
| 914 | 911.2 |
| 2617 | 2614.6 |
slope=1.0003 +/- 0.000156023 y-intercept=-3.12645 +/- 0.185346
MPA->Draw("-3.12645+1.0003*evt.Chan>>(8000,0,8000)");
Scotch tape run was 6663.4 seconds long (MPA->Draw("-3.12645+1.0003*evt.Chan>>NScotchTape(8000,0,8000)","0.00015");)
Kapton Tape run was 488.44 seconds long (MPA->Draw("-3.12645+1.0003*evt.Chan>>NKaptonTape(8000,0,8000)","0.0020473344");)
HEU disks
A 20 MeV electron was used to make a bremsstrahlung beam that impinged HEU disks
Below is an uncalibrated spectrum using Thorium rods on Detector D. Lines should appear at 238.8,338.8, 511, 583.4, 911.2, and 2614.6 keV
The HEU samples were measured on two different HpGe detectors that has similar efficiencies. Get B was used for the Unirradiate sample and Detector D for the Irradiated HEU disk.
Det D calibrations
| Channel | Energy (keV) |
| 236 | 238.8 |
| 334 | 338.8 |
| 505 | 511 |
| 576 | 583 |
| 901 | 911.2 |
| 2586 | 2614.6 |
slope=1.0108 +/- 0.000328475 y-intercept=0.6533 +/- 0.385247
MPA->Draw("0.6533+1.0108*evt.Chan>>(8000,0,8000)");
HEU comparison Before and After irradiation
Uniradiated HEU sample was measured for 2671.8 seconds
MPA->Draw("-3.12645+1.0003*evt.Chan>>NHEUback(2000,0,8000)","0.0003742795");
Iradiated HEU sample was measured overnight for 50554.469 seconds (14 hours)
MPA->Draw("0.6533+1.0108*evt.Chan>>NIradHEU(2000,0,8000)","0.00001978064");