September 19, 2011 - Revision history

Shaproma at 14:10, 20 September 2011

2011-09-20T14:10:15Z

← Older revision		Revision as of 14:10, 20 September 2011
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	[https://wiki.iac.isu.edu/index.php?title=September_19,_2011~~&action=edit~~ Go up]		[https://wiki.iac.isu.edu/index.php?title=September_19,_2011 Go up]

Shaproma at 14:09, 20 September 2011

2011-09-20T14:09:07Z

← Older revision		Revision as of 14:09, 20 September 2011
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	[https://wiki.iac.isu.edu/index.php~~/Sept_PhotFisRun_44MeV_2011#Log_eBook~~ Go ~~Back~~]		[https://wiki.iac.isu.edu/index.php?title=September_19,_2011&action=edit Go up]

Shaproma: /* Summary of the day */

2011-09-20T00:24:00Z

Summary of the day

← Older revision		Revision as of 00:24, 20 September 2011
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	R(upstream) = 0.01393 = e+/pulse<br>		R(upstream) = 0.01393 = e+/pulse<br>
	\|-		\|-
	\|<span style="color:blue">'''2499'''</span>\|\|Down<br> 86A\|\|In \|\|Open \|\|~~Out~~ \|\|Yes \|\|Out\|\|DU cylinder		\|<span style="color:blue">'''2499'''</span>\|\|Down<br> 86A\|\|In \|\|Open \|\|In \|\|Yes \|\|Out\|\|DU cylinder
	\|align="left"\|<span style="color:blue">'''Long production run'''</span>		\|align="left"\|<span style="color:blue">'''Long production run'''</span>
	R(beam down) = 0 n/pulse <span style="color:blue"> -> ×180×60 = '''0 n/min'''</span><br>		R(beam down) = 0 n/pulse <span style="color:blue"> -> ×180×60 = '''0 n/min'''</span><br>
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	<span style="color:blue">About '''93%''' of photons are coming from the radiator according to PS. Very Good</span><br>		<span style="color:blue">About '''93%''' of photons are coming from the radiator according to PS. Very Good</span><br>
	\|-		\|-
	\|<span style="color:blue">'''2500'''</span>\|\|Down<br> 86A\|\|In \|\|Open \|\|~~Out~~ \|\|Yes \|\|In\|\|Out		\|<span style="color:blue">'''2500'''</span>\|\|Down<br> 86A\|\|In \|\|Open \|\|In \|\|Yes \|\|In\|\|Out
	\|align="left"\|<span style="color:blue">'''Long production run'''</span>. Beam off		\|align="left"\|<span style="color:blue">'''Long production run'''</span>. Beam off
	\|-		\|-
	\|<span style="color:blue">'''2501'''</span>\|\|Down<br> 86A\|\|In \|\|Open \|\|~~Out~~ \|\|Yes \|\|In\|\|Out		\|<span style="color:blue">'''2501'''</span>\|\|Down<br> 86A\|\|In \|\|Open \|\|In \|\|Yes \|\|In\|\|Out
	\|align="left"\|<span style="color:blue">'''Long production run'''</span>.		\|align="left"\|<span style="color:blue">'''Long production run'''</span>.
	R(beam down) = 0.000026 n/pulse <span style="color:blue"> -> ×180×60 = '''0.28 n/min'''</span><br>		R(beam down) = 0.000026 n/pulse <span style="color:blue"> -> ×180×60 = '''0.28 n/min'''</span><br>

Shaproma: /* Summary of the day */

2011-09-20T00:21:42Z

Summary of the day

@@ Line 27: / Line 27: @@
 R(beam down) = 0.000018 n/pulse  <br>
 R(upstream) = 0.00116 = e+/pulse<br>
-<span style="color:red">About '''93%''' of photons are coming from the radiator according to PS. Good</span><br>
+<span style="color:red">About '''93%''' of photons are coming from the radiator according to PS. Very Good</span><br>
 |-
 |<span style="color:red">'''2482'''</span>||Down<br> 86A||In ||Open ||Yes ||In||DU cylinder
@@ Line 61: / Line 61: @@
 R(beam down) = 0.00057 n/pulse  <br>
 R(upstream) = 0.0129 = e+/pulse<br>
-<span style="color:red">About '''91%''' of photons are coming from the radiator according to PS. Good</span><br>
+<span style="color:red">About '''91%''' of photons are coming from the radiator according to PS. Very Good</span><br>
 |-
 |<span style="color:red">'''2490'''</span>||Up<br> 90A||In ||Open ||Yes ||In||DU cylinder
@@ Line 75: / Line 75: @@
 R(beam down) = 0 n/pulse  <br>
 R(upstream) = 0.00080 = e+/pulse<br>
-<span style="color:red">About '''93%''' of photons are coming from the radiator according to PS. Good</span><br>
+<span style="color:red">About '''93%''' of photons are coming from the radiator according to PS. Very Good</span><br>
 |-
 |}
@@ Line 99: / Line 99: @@
 R(upstream) = 0.0142 = e+/pulse<br>
 |-
 |}

Shaproma: /* Summary of the day */

2011-09-20T00:09:14Z

Summary of the day

← Older revision		Revision as of 00:09, 20 September 2011
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	\|<span style="color:blue">'''2494'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|In \|\|Yes \|\|In\|\|DU cylinder		\|<span style="color:blue">'''2494'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|In \|\|Yes \|\|In\|\|DU cylinder
	\|align="left"\|<span style="color:blue">'''Long production run'''</span>		\|align="left"\|<span style="color:blue">'''Long production run'''</span>
	190006 pulses<br>		<span style="color:blue">'''190006 pulses'''</span><br>
	R(beam down) = 0.00063 n/pulse <span style="color:blue"> -> ×180×60 = '''6.8 n/min'''</span><br>		R(beam down) = 0.00063 n/pulse <span style="color:blue"> -> ×180×60 = '''6.8 n/min'''</span><br>
	R(upstream) = 0.0142 = e+/pulse<br>		R(upstream) = 0.0142 = e+/pulse<br>

Shaproma: /* Summary of the day */

2011-09-20T00:07:27Z

Summary of the day

← Older revision		Revision as of 00:07, 20 September 2011
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	Good beam, good turning. So there are <span style="color:blue">'''~~2492~~'''~~production runs~~</span>		Good beam, good turning. So there are <span style="color:blue">'''production runs'''</span>

	{\| border="1" cellspacing="0" style="text-align: center; width: 1000px "		{\| border="1" cellspacing="0" style="text-align: center; width: 1000px "
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	\|<span style="color:blue">'''2494'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|In \|\|Yes \|\|In\|\|DU cylinder		\|<span style="color:blue">'''2494'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|In \|\|Yes \|\|In\|\|DU cylinder
	\|align="left"\|<span style="color:blue">'''Long production run'''</span>		\|align="left"\|<span style="color:blue">'''Long production run'''</span>
	190006 pulses</br>		190006 pulses<br>
	R(beam down) = 0.00063 n/pulse <span style="color:blue"> -> ×180×60 = '''6.8 n/min'''</span><br>		R(beam down) = 0.00063 n/pulse <span style="color:blue"> -> ×180×60 = '''6.8 n/min'''</span><br>
	R(upstream) = 0.0142 = e+/pulse<br>		R(upstream) = 0.0142 = e+/pulse<br>

Shaproma: /* Summary of the day */

2011-09-20T00:06:45Z

Summary of the day

← Older revision		Revision as of 00:06, 20 September 2011
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	! scope="col" width="7.2%" \| Dump magnet		! scope="col" width="7.2%" \| Dump magnet
	! scope="col" width="7.2%" \| Collimator		! scope="col" width="7.2%" \| Collimator
			! scope="col" width="7.2%" \| add coll
	! scope="col" width="7.2%" \| Hardener 1" Al		! scope="col" width="7.2%" \| Hardener 1" Al
	! scope="col" width="7.2%" \| Radiator 10 um Al		! scope="col" width="7.2%" \| Radiator 10 um Al
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	! scope="col" width="56.6%" \| Comments		! scope="col" width="56.6%" \| Comments
	\|-		\|-
	\|<span style="color:blue">'''2494'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|Yes \|\|In\|\|DU cylinder		\|<span style="color:blue">'''2494'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|In \|\|Yes \|\|In\|\|DU cylinder
	\|align="left"\|~~Additional collimator in. '''Long production run'''</span>~~		\|align="left"\|<span style="color:blue">'''Long production run'''</span>
	~~190006 pulses~~		190006 pulses</br>
	~~R(beam down) = 0.00063 n/pulse~~ <span style="color:blue"> ~~-> ×180×60 = '''6.8 n/min'''</span><br>~~
	~~R(upstream) = 0.0142 = e+/pulse<br>~~
	\|-
	~~\|<span style="color:blue">'''2494'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|Yes \|\|In\|\|DU cylinder~~
	~~\|align="left"\|Additional collimator in.~~ '''Long production run'''</span>
	190006 pulses
	~~R(beam down) = 0.00063 n/pulse <span style="color:blue"> -> ×180×60 = '''6.8 n/min'''</span><br>~~
	~~R(upstream) = 0.0142 = e+/pulse<br>~~
	\|-
	~~\|<span style="color:blue">'''2494'''~~</~~span>\|\|Up<~~br> ~~90A\|\|In \|\|Open \|\|Yes \|\|In\|\|DU cylinder~~
	~~\|align="left"\|Additional collimator in. '''Long production run'''</span>~~
	~~190006 pulses~~
	R(beam down) = 0.00063 n/pulse <span style="color:blue"> -> ×180×60 = '''6.8 n/min'''</span><br>		R(beam down) = 0.00063 n/pulse <span style="color:blue"> -> ×180×60 = '''6.8 n/min'''</span><br>
	R(upstream) = 0.0142 = e+/pulse<br>		R(upstream) = 0.0142 = e+/pulse<br>

Shaproma at 00:04, 20 September 2011

2011-09-20T00:04:38Z

@@ Line 76: / Line 76: @@
 R(upstream) = 0.00080 = e+/pulse<br>
 <span style="color:red">About '''93%''' of photons are coming from the radiator according to PS. Good</span><br>
 |-

Shaproma: /* Summary of the day */

2011-09-19T23:57:46Z

Summary of the day

← Older revision		Revision as of 23:57, 19 September 2011
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	\|align="left"\|Beam check-in run. Beam lost.		\|align="left"\|Beam check-in run. Beam lost.
	R(beam down) n/pulse <br>		R(beam down) n/pulse <br>
	R(upstream) = = e+/pulse<br>		R(upstream) e+/pulse<br>
	\|-		\|-
	\|}		\|}
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	R(upstream) = 0.01198 = e+/pulse<br>		R(upstream) = 0.01198 = e+/pulse<br>
	\|-		\|-
	\|<span style="color:red">'''2492'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|Yes \|\|In\|\|DU cylinder		\|<span style="color:red">'''2492'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|Yes \|\|Out\|\|DU cylinder
	\|align="left"\|Beam check-in run.		\|align="left"\|Beam check-in run.
	R(beam down) = 0 n/pulse <br>		R(beam down) = 0 n/pulse <br>

Shaproma: /* Summary of the day */

2011-09-19T23:53:46Z

Summary of the day

← Older revision		Revision as of 23:53, 19 September 2011
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	\|-		\|-
	\|<span style="color:red">'''2483'''</span>\|\|Down<br> 86A\|\|In \|\|Open \|\|Yes \|\|Out\|\|DU cylinder		\|<span style="color:red">'''2483'''</span>\|\|Down<br> 86A\|\|In \|\|Open \|\|Yes \|\|Out\|\|DU cylinder
	\|align="left"\|Beam check-in run.		\|align="left"\|Beam check-in run. Beam lost.
	R(beam down) n/pulse <br>		R(beam down) n/pulse <br>
	R(upstream) = = e+/pulse<br>		R(upstream) = = e+/pulse<br>
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	\|-		\|-
	\|<span style="color:red">'''2488'''</span>\|\|Down<br> 86A\|\|In \|\|Open \|\|Yes \|\|Out\|\|DU cylinder		\|<span style="color:red">'''2488'''</span>\|\|Down<br> 86A\|\|In \|\|Open \|\|Yes \|\|Out\|\|DU cylinder
	\|align="left"\|Beam check-in run. Additional collimator in		\|align="left"\|Beam returned without VS. Beam check-in run. Additional collimator in
	R(beam down) = 0 n/pulse <br>		R(beam down) = 0 n/pulse <br>
	R(upstream) = 0.00116 = e+/pulse<br>		R(upstream) = 0.00116 = e+/pulse<br>
			\|-
			\|<span style="color:red">'''2489'''</span>\|\|Down<br> 86A\|\|In \|\|Open \|\|Yes \|\|In\|\|DU cylinder
			\|align="left"\|Beam check-in run.
			R(beam down) = 0.00057 n/pulse <br>
			R(upstream) = 0.0129 = e+/pulse<br>
			<span style="color:red">About '''91%''' of photons are coming from the radiator according to PS. Good</span><br>
			\|-
			\|<span style="color:red">'''2490'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|Yes \|\|In\|\|DU cylinder
			\|align="left"\|Beam off.
			\|-
			\|<span style="color:red">'''2491'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|Yes \|\|In\|\|DU cylinder
			\|align="left"\|Beam check-in run.
			R(beam down) = 0.000569 n/pulse <br>
			R(upstream) = 0.01198 = e+/pulse<br>
			\|-
			\|<span style="color:red">'''2492'''</span>\|\|Up<br> 90A\|\|In \|\|Open \|\|Yes \|\|In\|\|DU cylinder
			\|align="left"\|Beam check-in run.
			R(beam down) = 0 n/pulse <br>
			R(upstream) = 0.00080 = e+/pulse<br>
			<span style="color:red">About '''93%''' of photons are coming from the radiator according to PS. Good</span><br>
	\|-		\|-