By Kroh M.
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The ebook is a commemorative quantity honoring the mathematician Paul R. Halmos (1916-2006), who contributed passionately to arithmetic in manifold methods, between them by way of easy examine, by means of remarkable mathematical exposition, through unselfish carrier to the mathematical neighborhood, and, now not least, through the foundation others present in his commitment to that neighborhood.
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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 .
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