A Guide to the Sacz Ethnographic Park. by Kroh M.

By Kroh M.

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Typical parameters of CUORE NTDs are: R0 ¼ 1:15 X; T0 ¼ 3:35 K and c ¼ 1=2 ð2:15Þ Using these values we can calculate the static resistance (RS ) at the working temperature TS ¼ 10 mK to be approximately 100 MX. 2 Bolometer Operation To measure the resistance variation the thermistor is biased with the circuit shown in Fig. 3a. 2 Bolometer Operation 25 logR RL/2 20 VBIAS + Ibol R(T) Vbol(T) 4 2 RL/2 Temperature 10 8 6 1 10-2 (a) 102 1 104 106 P [pW] (b) Fig. 3 Picture a shows the electric scheme of the bias circuit used for thermistor readout.

In the VRH conduction regime the resistivity dependence on temperature is described by the law: Fig. 2 Schematic representation of the hopping conduction mechanism phonon electron tunneling e Energy e e hopping length donor atom site donor atom site 24 2 TeO2 Bolometric Detectors for 0mDBD Search  c T0 qðTÞ ¼ q0 exp T ð2:12Þ where q0 , T0 depend on the doping concentration and c ¼ 1=2. 4 NTD-Ge Thermistors The thermal sensor used in CUORICINO and CUORE bolometers is a Neutron Transmutation Doped (NTD)germanium thermistor operating in the VRH regime [9].

13, 31 (1990) 33. : Mod. Phys. Lett. A16, 2409 (2001). 1142/S0217732301005825 34. : Nucl. Instrum. Meth. A536, 79 (2005). 194 References 17 35. : Nucl. Phys. A766, 107 (2006). 004 36. : arXiv:hep-ex/0404039v1 (2004) 37. , et al. 2446v1 [nucl-ex] (2008) 38. , et al. [Majorana collaboration]: arXiv:nucl-ex/0311013v1 (2003) 39. : Nucl. Instrum. Meth. A518, 775 (2004). nima. 067 40. : arXiv:hep-ex/0501010v1 (2005) 41. : Phys. Atom. Nucl. 69, 2096 (2006). 1134/S1063778806120131 42. : Phys. Lett. B480, 12 (2000).

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