Difference between revisions of "Experimental setup"
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'''Figure 4''': This new architecture is used for obtaining timing spectra during runs 60 - 63 (http://www.iac.isu.edu/mediawiki/index.php/Timing_spectra), <math>P_B = 3.97 Torr</math>, <math>P_C = 4.5 Torr</math>. | '''Figure 4''': This new architecture is used for obtaining timing spectra during runs 60 - 63 (http://www.iac.isu.edu/mediawiki/index.php/Timing_spectra), <math>P_B = 3.97 Torr</math>, <math>P_C = 4.5 Torr</math>. | ||
− | [[Image: | + | [[Image:exp_setup6_2.jpg]] |
'''Figure 5''': Beam produces nuclear fragments on <math>C^{12}</math> and Al and fission fragments on <math>U^{235}</math>. P = 4.96 Torr (heptane), <math>N_{T1} \sim 4.6/100 sec</math> (beam off), <math>N_{T1} \sim 2.75/100 sec</math> (beam on!). Chambers are not stable due to vacuum leak. | '''Figure 5''': Beam produces nuclear fragments on <math>C^{12}</math> and Al and fission fragments on <math>U^{235}</math>. P = 4.96 Torr (heptane), <math>N_{T1} \sim 4.6/100 sec</math> (beam off), <math>N_{T1} \sim 2.75/100 sec</math> (beam on!). Chambers are not stable due to vacuum leak. |
Revision as of 22:56, 17 April 2008
Collimator parameters: in upstream side of wall 5/8
3/4", in downstream side of wall 1/2".Figure 1: 8:21 am -
pulse, 200 ns, 300 Hz, of beam, 6 fissions. 9:10 am - Threshold 80 mV, .Figure 2:
, , , , . , . Geometrical dimensions for detector placement and chamber size are the same as in Figure 1.Figure 3:
, , , , . , threshold = 80 mV, . Geometrical dimensions for detector placement and chamber size are the same as in Figure 1.Figure 4:
, , , , . , , threshold = 80 mV, . Geometrical dimensions for detector placement and chamber size are the same as in Figure 1.Figure 4: This new architecture is used for obtaining timing spectra during runs 60 - 63 (http://www.iac.isu.edu/mediawiki/index.php/Timing_spectra), , .
Figure 5: Beam produces nuclear fragments on http://www.iac.isu.edu/mediawiki/index.php/Energy_spectra_%28fiss_frag%29).
and Al and fission fragments on . P = 4.96 Torr (heptane), (beam off), (beam on!). Chambers are not stable due to vacuum leak. If nothing was changed this geometry was used to get all the energy spectra (Figure 6: ADC distributions of
(left) and (right). Data obtained via experimental setup shown in Figure 5.