Testing of bulk radiation damage of n-in-p silicon sensors for very high radiation environments

We are developing n +-in-p, p-bulk and n-readout, microstrip sensors, fabricated by Hamamatsu Photonics, as a non-inverting radiation hard silicon detector for the ATLAS tracker upgrade at the super-LHC (sLHC) proposed facility. The bulk radiation damage after neutron and proton irradiations is char...

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Published in:Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Vol. 636; no. 1; pp. S83 - S89
Main Authors: Hara, K., Affolder, A.A., Allport, P.P., Bates, R., Betancourt, C., Bohm, J., Brown, H., Buttar, C., Carter, J.R., Casse, G., Chen, H., Chilingarov, A., Cindro, V., Clark, A., Dawson, N., DeWilde, B., Doherty, F., Dolezal, Z., Eklund, L., Fadeyev, V., Ferrere, D., Fox, H., French, R., García, C., Gerling, M., Gonzalez Sevilla, S., Gorelov, I., Greenall, A., Grillo, A.A., Hamasaki, N., Hatano, H., Hoeferkamp, M., Hommels, L.B.A., Ikegami, Y., Jakobs, K., Kierstead, J., Kodys, P., Köhler, M., Kohriki, T., Kramberger, G., Lacasta, C., Li, Z., Lindgren, S., Lynn, D., Maddock, P., Mandić, I., Martinez-McKinney, F., Martí i Garcia, S., Maunu, R., McCarthy, R., Metcalfe, J., Mikestikova, M., Mikuž, M., Miñano, M., Mitsui, S., O'Shea, V., Parzefall, U., Sadrozinski, H.F.-W., Schamberger, D., Seiden, A., Terada, S., Paganis, S., Robinson, D., Puldon, D., Sattari, S., Seidel, S., Takahashi, Y., Toms, K., Tsionou, D., Unno, Y., Von Wilpert, J., Wormald, M., Wright, J., Yamada, M.
Format: Journal Article
Language:English
Published: Elsevier B.V 21-04-2011
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Summary:We are developing n +-in-p, p-bulk and n-readout, microstrip sensors, fabricated by Hamamatsu Photonics, as a non-inverting radiation hard silicon detector for the ATLAS tracker upgrade at the super-LHC (sLHC) proposed facility. The bulk radiation damage after neutron and proton irradiations is characterized with the leakage current, charge collection and full depletion voltage. The detectors should provide acceptable signal, signal-to-noise ratio exceeding 15, after the integrated luminosity of 6000 fb −1, which is twice the sLHC integrated luminosity goal.
ISSN:0168-9002
1872-9576
DOI:10.1016/j.nima.2010.04.090