Difference between revisions of "Experimental setup"

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'''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.
If nothing was changed this geometry was used to get all the energy spectra (http://www.iac.isu.edu/mediawiki/index.php/Energy_spectra_%28fiss_frag%29)
+
If nothing was changed this geometry was used to get all the energy spectra (http://www.iac.isu.edu/mediawiki/index.php/Energy_spectra_%28fiss_frag%29).
  
 
[[Image:results_for_setup6.jpg]]
 
[[Image:results_for_setup6.jpg]]
  
 
'''Figure 6''': ADC distributions of <math>T_2</math> (left) and <math>T_1</math> (right). Data obtained via experimental setup shown in Figure 5.
 
'''Figure 6''': ADC distributions of <math>T_2</math> (left) and <math>T_1</math> (right). Data obtained via experimental setup shown in Figure 5.

Revision as of 20:10, 17 April 2008

Collimator parameters: in upstream side of wall 5/8 [math]\rightarrow[/math] 3/4", in downstream side of wall 1/2".

Exp setup1.jpg

Figure 1: 8:21 am - [math]40 mAmps[/math] pulse, 200 ns, 300 Hz, [math]10^3 secs[/math] of beam, 6 fissions. 9:10 am - Threshold 80 mV, [math]N_{T1} = 17.6 counts/10 min[/math].

Exp setup2.jpg

Figure 2: [math]\Delta T = 200 ns[/math], [math]I_e = 40 mA[/math], [math]f = 300 Hz[/math], [math]E_e = 20 MeV[/math], [math]q = 8.7 nC/pulse[/math]. [math]N_{T1} = 12 counts/10 min[/math], [math]N_{T2} = 35 counts/10 min[/math]

Exp setup3.jpg

Figure 3: [math]\Delta T = 200 ns[/math], [math]I_e = 40 mA[/math], [math]f = 300 Hz[/math], [math]E_e = 20 MeV[/math], [math]q = 8.7 nC/pulse[/math]. [math]N_{T2} = 46 counts/10 min[/math], threshold = 80 mV, [math]P_B = 33.9[/math]

Exp setup4.jpg

Figure 4: [math]\Delta T = 200 ns[/math], [math]I_e = 40 mA[/math], [math]f = 300 Hz[/math], [math]E_e = 20 MeV[/math], [math]q = 8.7 nC/pulse[/math]. [math]N_{T2} \sim 48 counts/10 min[/math], [math]N_{T1} (thresh = 30 mV, beam on) = 1065 counts/10 min[/math], threshold = 80 mV, [math]P_B = 33.9[/math]


Exp setup5.jpg

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].

Exp setup6.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. If nothing was changed this geometry was used to get all the energy spectra (http://www.iac.isu.edu/mediawiki/index.php/Energy_spectra_%28fiss_frag%29).

Results for setup6.jpg

Figure 6: ADC distributions of [math]T_2[/math] (left) and [math]T_1[/math] (right). Data obtained via experimental setup shown in Figure 5.