CaGaS Phase II - Revision history

Harpconn: /* V) CaGaS Phase II */

2022-12-01T22:21:46Z

V) CaGaS Phase II

Harpconn: /* To Do */

2022-12-01T22:21:25Z

To Do

Harpconn: /* IV) HPGe Measurements */

2022-11-21T18:05:42Z

IV) HPGe Measurements

Harpconn: /* To Do */

2022-11-21T17:43:03Z

To Do

Harpconn: /* Electronics Chain */

2022-11-21T16:24:52Z

Electronics Chain

Harpconn: /* To Do */

2022-11-21T16:24:40Z

To Do

Harpconn: /* Impromptu To Do List */

2022-11-21T16:24:19Z

Impromptu To Do List

Harpconn: /* Impromptu To Do List */

2022-11-21T16:24:03Z

Impromptu To Do List

Harpconn: /* Impromptu To Do List */

2022-11-21T16:23:31Z

Impromptu To Do List

Harpconn: /* III) CaGaS Phase I Expansion */

2022-11-21T16:17:16Z

III) CaGaS Phase I Expansion

← Older revision		Revision as of 22:21, 1 December 2022
Line 50:		Line 50:

	='''V) CaGaS Phase II'''=		='''V) CaGaS Phase II'''=
−
−	~~[[CH Phase II Run Plan]]~~

	='''Previous Work'''=		='''Previous Work'''=

← Older revision		Revision as of 22:21, 1 December 2022
Line 1:		Line 1:
	<big>'''CaGaS Phase II (Capture Gamma Spectroscopy) is a repeat of capture gamma energy spectroscopy experiments performed during the summer of 2021 in the ISU clean room. The purpose of revisiting the capture gamma experiment is to use a new, higher activity <sup>252</sup>Cf source (U2-622) and to investigate different thicknesses of Gadolinium foils and the effect on the high energy photon flux produced. This work is being performed in support of the main conversion process for the In-Situ Positron Annihilation Spectroscopy experiment being designed and performed by INL staff and external collaborators.'''</big>		<big>'''CaGaS Phase II (Capture Gamma Spectroscopy) is a repeat of capture gamma energy spectroscopy experiments performed during the summer of 2021 in the ISU clean room. The purpose of revisiting the capture gamma experiment is to use a new, higher activity <sup>252</sup>Cf source (U2-622) and to investigate different thicknesses of Gadolinium foils and the effect on the high energy photon flux produced. This work is being performed in support of the main conversion process for the In-Situ Positron Annihilation Spectroscopy experiment being designed and performed by INL staff and external collaborators.'''</big>
−
−	~~='''To Do'''=~~
−
−	*Measure up as close to Gd as possible and then ~12" away to calculate the adjustment factors necessary for coincidences

	='''Weekly Reports'''=		='''Weekly Reports'''=

@@ Line 45: / Line 45: @@
 [[CH He3 Attenuation Measurements: 3 Different Cf252 Sources]]
-='''IV) HPGe Measurements'''=
+='''IV) HPGe'''=
 [[PAS HPGe Detector]]

← Older revision		Revision as of 17:43, 21 November 2022
Line 4:		Line 4:

	*Measure up as close to Gd as possible and then ~12" away to calculate the adjustment factors necessary for coincidences		*Measure up as close to Gd as possible and then ~12" away to calculate the adjustment factors necessary for coincidences
		+
		+	='''Weekly Reports'''=
		+
		+	[[CH Weekly Reports]]

	='''I) CaGaS Phase II Associated Equipment and Experimental Setup'''=		='''I) CaGaS Phase II Associated Equipment and Experimental Setup'''=

← Older revision		Revision as of 16:24, 21 November 2022
Line 20:		Line 20:

	[[CH_HPGe_Electronics_Chain]]		[[CH_HPGe_Electronics_Chain]]
		+
		+	[[CH_785NADC]]

	=='''Gadolinium'''==		=='''Gadolinium'''==

@@ Line 1: / Line 1: @@
 <big>'''CaGaS Phase II (Capture Gamma Spectroscopy) is a repeat of capture gamma energy spectroscopy experiments performed during the summer of 2021 in the ISU clean room. The purpose of revisiting the capture gamma experiment is to use a new, higher activity <sup>252</sup>Cf source (U2-622) and to investigate different thicknesses of Gadolinium foils and the effect on the high energy photon flux produced. This work is being performed in support of the main conversion process for the In-Situ Positron Annihilation Spectroscopy experiment being designed and performed by INL staff and external collaborators.'''</big>
-='''Impromptu To Do List'''=
+='''To Do'''=
 *Measure up as close to Gd as possible and then ~12" away to calculate the adjustment factors necessary for coincidences

@@ Line 6: / Line 6: @@
 **Look for differences with high count rate source
-*Build shielded tunnel for Gd optimal thickness measurements
+*Measure up as close to Gd as possible and then ~12" away to calculate the adjustment factors necessary for coincidences
 [[CH_785NADC]]

@@ Line 10: / Line 10: @@
 **Design and print holders for foils and powder
 **Measure up as close to Gd as possible and then ~12" away to calculate the adjustment factors necessary for coincidences
 [[CH_785NADC]]

← Older revision		Revision as of 16:17, 21 November 2022
Line 57:		Line 57:

	[[CH He3 Attenuation Measurements: 3 Different Cf252 Sources]]		[[CH He3 Attenuation Measurements: 3 Different Cf252 Sources]]
−
−	~~='''III) CaGaS Phase I Expansion'''=~~
−
−	~~[[CaGaS Phase I Gadolinium]]~~
−
−	~~[[CaGaS Phase I Cadmium]]~~

	='''IV) HPGe Measurements'''=		='''IV) HPGe Measurements'''=