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Rainer Schicker, Univ. Heidelberg Cheile Gradistei, sept 26, 2005
Status chamber testing/database
• Chamber testing procedures finalized may 13
– See manual Vers. 5 in forum.gsi.de/Alice/TRD chamber tests
• Use of 109Cd source in testing
• Database
Rainer Schicker, Univ. Heidelberg Cheile Gradistei, sept 26, 2005
55Fe source
• 55Fe EC to 55Mn, K = 5.9, 6.5 keV
T.Lehmann, 2003
Transmission radiator at 5.9 keV is about 1%
Rainer Schicker, Univ. Heidelberg Cheile Gradistei, sept 26, 2005
55Fe source for gain uniformity
• N0 = photon flux from the source • A = absorption in radiator
• A = variation in absorption (radiator thickness,glue,..)
• Ns = number of photons into gas volume
Ns = N0 x (1-A)
Ns) = dNsdN0
.(N0) + dNsdA
. (A)
(Ns) Ns
N0~Ns
.(A)
(Ns)Ns
~ (A/1-A)(A)
A
for A ~ 0.99: (A/1-A) ~ 100
for A ~ 0.5: (A/1-A) ~ 1
Rainer Schicker, Univ. Heidelberg Cheile Gradistei, sept 26, 2005
absorption radiator
• Absorption measured as function of energy
T. Lehmann, 2003
transmission > 50 %:-> E(photon) > 10 keV
Source parameters:1) photon energy2) life time 3) no neutrons
-> 109Cd
Rainer Schicker, Univ. Heidelberg Cheile Gradistei, sept 26, 2005
109Cd source (453 d)
• 109Cd EC to 109Ag, K = 22.9, 26.0 keV
K
K
Ag*(7/2 +),E=88 keV
Collimator:Absorption (1mm Pb)at 88 keV ~ 90 %
Rainer Schicker, Univ. Heidelberg Cheile Gradistei, sept 26, 2005
109Cd spectrum
• 109Cd spectrum measured with TRD chamber
2nd peak at approx. 8 keV-> compatible with E(K of Z~29 (copper)
Confirmation by AEA: Casing material monel( 1/3 copper, 2/3 nickel)
Information by AEA: Casing material could be Titanium, (Z=22),E(K ~ 4.5 keV),Cd contains Silikat (Na-Al)
Rainer Schicker, Univ. Heidelberg Cheile Gradistei, sept 26, 2005
1d scan X-ray vs 109Cd source
• L1C1#020 measured with X-ray tube, Cd source
X-ray scan
Cd scan
Rainer Schicker, Univ. Heidelberg Cheile Gradistei, sept 26, 2005
2d scan X-ray vs 109Cd source
• L1C1#020 measured with X-ray tube, Cd source
X-ray scan
Cd scan
Rainer Schicker, Univ. Heidelberg Cheile Gradistei, sept 26, 2005
Conclusions
• 109Cd source can be used for measuring– Gain uniformity– Absolute Gain– Gain stability
• Absolute gain measurement has to be done with care with present Cd source (intensity 2nd peak might be collimation dependent)
-> Cd source with Titanium casing
Rainer Schicker, Univ. Heidelberg Cheile Gradistei, sept 26, 2005
Status database
• Sascha Freuen has graduated and left sep 15• Stefan Zimmer has started as HiWi and taken
over the database, no other involvement in TRD activities
• As of sep 22, writing of some leak rate parameters to database successful