Published December 1992 | Version v1
Report

Calorimetric particle detectors with superconducting absorber materials

  • 1. Technische Univ. Muenchen, Garching (Germany). Physik-Department E15

Description

We use massive superconducting absorbers made of Molybdenum and Vanadium as low temperature calorimetric particle detectors. The high resolution of our thermometry system, consisting of a superconducting phase transition thermometer monitored with a dc-SQUID, enables us to detect α and γ particles with large single crystals. Heat pulses generated by passing current through a metal film on the surface of the crystal are used to study the response of the calorimeters. With a 35 g Molybdenum single crystal we obtain an energy resolution of 10% FWHM on 5.8 MeV α particles at an operating temperature of 120 mK. The observed temperature rise of 1.2 μK is a factor of eight less than expected from the calculated heat capacity. Using a 15 g Vanadium single crystal, the energy resolution on 5.8 MeV α particles is 1.2% FWHM. In this case, the pulse height of 6.1 μK is a factor of eight smaller than expected from the calculated heat capacity. A possible reason for the large deviations from the expected heat capacity is the response of hydrogen dissolved in Vanadium. Impurities and defects on the surface of the crystals probably also contribute to the heat capacity. The pulse shapes of all observed events are very similar, whether they are created by absorption of α or γ radiation or by an electrically created heat pulse, and consists of two exponential decaying parts. A comparison of the pulse heigths of heater and radiation pulses leads us to the conclusion that all the energy deposited in the absorber crystal is converted into phonons. (orig.)

Availability note (English)

Available from FIZ Karlsruhe.
Part of:
TUM-MPI cryogenic detector development 1992

Additional details

Publishing Information

Imprint Title
TUM-MPI cryogenic detector development 1992
Imprint Pagination
49 p.
Journal Page Range
p. 1-6.
Report number
MPI-PhE--92-24

Optional Information