References

  1. For reviews of the class of spectrometers called low-temperature detectors (of which calorimeters are one type) and of many of the applications discussed in the introductory portions of this article, see N. Booth, B. Cabrera, E. Fiorini, Annu. Rev. Nucl. Particle Sci. 46, 471 (1996) and D. Twerenbold, Rep. Prog. Phys. 59, 349 (1996).
  2. T. Shutt et al., Phys. Rev. Lett. 69, 3425 (1992).
  3. G. C. Hilton et al., Nature 391, 672 (1998).
  4. E. Fiorini, T. O. Niinikoski, Nucl. Instrum. Methods 224, 83 (1984).
  5. D. McCammon, M. Juda, D. D. Reeder, R. L. Kelley, S. H. Moseley, A. E. Szymkowiak, in Neutrino Mass and Low Energy Weak Interactions: Telemark, 1984, V. Barger, D. Cline, eds., World Scientific, Singapore (1985), p. 329.
  6. B. Cabrera, R. M. Clarke, P. Colling, A. J. Miller, S. Nam, R. W. Romani, Appl. Phys. Lett. 73, 735 (1998).
  7. S. H. Moseley, J. C. Mather, D. McCammon, J. Appl. Phys. 56, 1257 (1984).
  8. J. C. Mather, Appl. Opt. 21, 1125 (1982). J. C. Mather, Appl. Opt. 23, 584 (1984).
  9. B. I. Shklovskii, A. L. Efros, Electronic Properties of Doped Semiconductors Springer-Verlag, Berlin (1984).
  10. J. Zhang et al., Phys. Rev. B 57, 4472 (1998). N. Wang, F. C. Wellstood, B. Sadoulet, E. E. Haller, J. Beeman, Phys. Rev. B, 41, 3761 (1990).
  11. S. I. Han et al., Proc. SPIE 3445, 640 (1998).
  12. A. Zehnder, Phys. Rev. B 52, 12858 (1995). This paper approaches the problem from the perspective of optimizing superconducting tunnel junctions, for which the quasiparticle current is measured before complete thermalization occurs, but the paper's overview of the thermalization process is relevant to calorimeters with superconducting absorbers.
  13. W. J. Skocpol, M. R. Beasley, M. Tinkham, J. Appl. Phys. 45, 4054 (1974).
  14. K. D. Irwin, Appl. Phys. Lett. 66, 1998 (1995).

Quantum Calorimetry Index