Abstract
A total absorption Nal(TI) detector can be used to define the energy of an incident electron, or γ-ray, to a precision of I to 2 per cent in the range of 4 to 14 GeV.
Similar content being viewed by others
References
Kantz, A., and Hofstadter, H., Phys. Rev., 89, 3 (1952); Kantz, A., and Hofstadter, R., Nucleonics, 12, 36 (1954).
Berezin, S., Hofstadter, R., and Yearian, M. R., Bull. Amer. Phys. Soc., 7, 620 (1962); Berezin, S., Stanford University High Energy Physics Laboratory Report HEPL-424; Berezin, S., thesis, Stanford Univ. (1967).
Völkel, U., DESY Report 65/6 (July 1965); DESY Report 67/16 (May 1967).
Crannell, C. J., Phys. Rev., 161, 310 (1967).
Bathow, G., Freytag, E., and Tesch, E., DESY Report 66/13 (May 1966).
Zerby, C. D., and Moran, H. S., J. Appl. Phys., 34, 2445 (1963).
Heusch, C. A., Proc. Intern. Conf. Electron–Photon Interactions, Hamburg, II, 408 (1965).
Dally, E. B., and Hofstadter, R., Rev. Sci. Instrum., 39, 658 (1968); Stanford University High Energy Physics Laboratory Report HEPL-531; Dally, E. B., and Hofstadter, R., IEEE Trans., NS-15, 76 (1968); Stanford University High Energy Physics Laboratory Report HEPL-550.
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
HOFSTADTER, R., HUGHES, E., LAKIN, W. et al. Nal(TI) Total Absorption Detector for Electrons and γ-Rays at GeV Energies. Nature 221, 228–230 (1969). https://doi.org/10.1038/221228a0
Received:
Issue Date:
DOI: https://doi.org/10.1038/221228a0
- Springer Nature Limited