Epitaxial Si sensors at low temperatures: Non-linear effects

被引:0
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作者
P. Stefanyi
C. C. Zammit
P. Fozooni
M. J. Lea
G. Ensell
I. D. Hepburn
机构
[1] University of London,Department of Physics, Royal Holloway
[2] University of Southampton,Department of Electronics and Computer Science
[3] Mullard Space Science Laboratory,undefined
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关键词
Heat Sink; Thermal Model; Sensor Arrangement; Critical Voltage; Phonon Coupling;
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摘要
Cryogenic bolometric sensors made from epitaxially grown Si:As have been tested down to 40 mK. The sensors were grown by chemical vapour deposition with a doped layer 8.4 μm thick. The dopant concentration was measured using SIMS and was constant, ±1%, with an excellent box profile. Arsenic concentrations up to 7.5×1018 cm−3 were achieved. Above 100 mK the low power resistanceR(T) followed the variable range hopping law, or Efros-Shklovskii law for a Coulomb gap,R(T)=R0 exp(T0/T)1/2 withT0∼25 K, typically. A double sensor arrangement was used to measure the electronphonon coupling in the sensors and the phonon coupling to the heat sink. As the dc current bias through a sensor was increased, spontaneous voltage oscillations were observed across the sensor below 100 mK, which limited the sensitivity of the sensors in this region. These are circuit-limited oscillations between high and low resistance states. A phase diagram was established for the spatio-temporal coexistence of the two states, with a critical temperatureTc=115 mK. We show that this is an intrinsic phase transition within a thermal model of the electron-phonon coupling. For a resistance-temperature characteristic given by the Efros-Shklovskii law we findTc=0.00512T0, independent ofR0 and the coupling strength. This predictsTc=115±4 mK in this case. The model gives excellent agreement for the critical voltage and current, by assuming that the breakdown occurred via the formation of a filamentary region of high current density and high electron temperature. At higher currents, the response was temperature independent and given byI(E)=I(0) exp{−(E0/E)1/2} whereE is the average applied electric field andE0∼380 V/cm, in agreement with a thermal model which includes the phonon-phonon coupling to the heat sink.
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页码:107 / 133
页数:26
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