Difference between revisions of "Experimental setup"
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Collimator parameters: in upstream side of wall 1/2", in downstream side of wall 1(1/2)". | Collimator parameters: in upstream side of wall 1/2", in downstream side of wall 1(1/2)". | ||
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+ | [[Image:whole_exp_setup.jpg]] | ||
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+ | '''Figure 0''': sketch of experimental setup. | ||
[[Image:exp_setup1_1.jpg]] | [[Image:exp_setup1_1.jpg]] |
Latest revision as of 10:38, 25 August 2008
Collimator parameters: in upstream side of wall 1/2", in downstream side of wall 1(1/2)".
Figure 0: sketch of experimental setup.
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.