TY - JOUR
T1 - Test beam characterization of 3-D silicon pixel detectors
AU - Mathes, Markus
AU - Cristinziani, M.
AU - Da Via, C.
AU - Garcia-Sciveres, M.
AU - Einsweiler, K.
AU - Hasi, J.
AU - Kenney, C.
AU - Parker, S. I.
AU - Reuen, L.
AU - Ruspa, M.
AU - Velthuis, J.
AU - Watts, S.
AU - Wermes, Norbert
N1 - Funding Information:
Manuscript received June 20, 2008; revised August 18, 2008. Current version published December 31, 2008. This work was supported by the German Ministerium für Bildung, Wissenschaft, Forschung und Technologie (BMBF) under Contract no. 06 HA6PD1 and in part by the U.S. Department of Energy Office of Science under Contract No. DE-AC02-05CH11231.. M. Mathes, M. Cristinziani, L. Reuen, and N. Wermes are with the University of Bonn, Physikalisches Institut, Bonn D-53115, Germany (e-mail: [email protected]; [email protected]). J. Velthuis was with the Bonn University, Bonn D-53115, Germany. He is now with the University of Bristol, Bristol BS8 1TL, U.K. C. Da Via, J. Hasi, and S. Watts are with the Manchester University, Manchester, M13 9PL, U.K. S. Parker is with the University of Hawaii, Honolulu, HI 96822 USA. M. Ruspa is with the University Piemonte Orientale, Novara, Italy. She is also with the Instituto Nazionale Di Fisica, Torino 10125, Torino, Italy. C. Kenney is with the Molecular Biology Consortium, Chicago, IL 60612 USA. M. Garcia-Sciveres and K. Einsweiler are with the Lawrence Berkeley National Laboratory, Berkeley, CA 94720 USA. Digital Object Identifier 10.1109/TNS.2008.2005630 Fig. 1. (a) Schematic view of 3-D silicon structures (x and y dimensions and not to scale). 3-D view showing the p and n electrodes and the active edge; the distance s is 70.6 , d is 208 . (b) View from the top of one pixel cell showing the n and p electrodes and the metallization connecting electrodes of the same type. The bump bond pad is shown at the far right.
PY - 2008/12
Y1 - 2008/12
N2 - Three-dimensional (3-D) silicon detectors are characterized by cylindrical electrodes perpendicular to the surface and penetrate into the bulk material in contrast to standard Si detectors with planar electrodes on the top and bottom. This geometry renders them particularly interesting to be used in environments where standard silicon detectors have limitations, such as, for example, the radiation environment expected in an upgrade to the Large Hadron Collider at CERN. For the first time, several 3-D sensors were assembled as hybrid pixel detectors using the ATLAS-pixel front-end chip and readout electronics. Devices with different electrode configurations have been characterized in a 100 GeV pion beam at the CERN SPS. Here, we report results on unirradiated devices with three 3D electrodes per 50 $\,\times \,$400 $\mu {\rm m}^{2}$ pixel area. Full charge collection is obtained already with comparatively low bias voltages around 10 V. Spatial resolution with binary readout is obtained as expected from the cell dimensions. Efficiencies of 95.9%$ \pm$0.1% for tracks incident parallel to the electrodes and of 99.9%$ \pm$0.1% for tracks incident at 15 $^{\circ} $ are measured. The homogeneity and charge sharing of the efficiency over the pixel area are measured.
AB - Three-dimensional (3-D) silicon detectors are characterized by cylindrical electrodes perpendicular to the surface and penetrate into the bulk material in contrast to standard Si detectors with planar electrodes on the top and bottom. This geometry renders them particularly interesting to be used in environments where standard silicon detectors have limitations, such as, for example, the radiation environment expected in an upgrade to the Large Hadron Collider at CERN. For the first time, several 3-D sensors were assembled as hybrid pixel detectors using the ATLAS-pixel front-end chip and readout electronics. Devices with different electrode configurations have been characterized in a 100 GeV pion beam at the CERN SPS. Here, we report results on unirradiated devices with three 3D electrodes per 50 $\,\times \,$400 $\mu {\rm m}^{2}$ pixel area. Full charge collection is obtained already with comparatively low bias voltages around 10 V. Spatial resolution with binary readout is obtained as expected from the cell dimensions. Efficiencies of 95.9%$ \pm$0.1% for tracks incident parallel to the electrodes and of 99.9%$ \pm$0.1% for tracks incident at 15 $^{\circ} $ are measured. The homogeneity and charge sharing of the efficiency over the pixel area are measured.
KW - Pixel detectors
KW - Silicon radiation detectors
KW - Vertex detectors
UR - http://www.scopus.com/inward/record.url?scp=58849092737&partnerID=8YFLogxK
U2 - 10.1109/TNS.2008.2005630
DO - 10.1109/TNS.2008.2005630
M3 - Article
SN - 0018-9499
VL - 55
SP - 3731
EP - 3735
JO - IEEE Transactions on Nuclear Science
JF - IEEE Transactions on Nuclear Science
IS - 6
M1 - 4723835
ER -