Minimum Ionizing Particle Detector Based on p+n Junction SiC Diode

Article Preview

Abstract:

In this work ion-implanted p+/n diodes have been used as minimum ionizing particle (MIP) detectors. The diode structure is based on a 0.45 $m deep, NA = 4×1019 cm-3 doped p+ anode, ion implanted in an n-type epilayer with thickness equal to 55 $m and nominal donor doping ND = 2×1014 cm-3. The diode breakdown voltages were above 1000V. At 1000V reverse bias the diode leakage current was of the order of 1 nA. The punch through depletion voltage was nearing the range 220-250 V. The charge collection efficiency to minimum ionizing particle was investigated by a 90Sr β source. The pulse height spectrum was measured as a function of the reverse voltage in the range 0-605 V. At each bias point the signal was stable and reproducible, showing the absence of polarization effects. At 220 V the collected charge was 2970 e- and saturated at 3150 e- near 350 V. At the moment, this is the highest collected charge for SiC detectors. At bias voltages over 100V the spectrum was found to consist of two peaks clearly separated. Around 250 V the signal saturates, in agreement with CV results.

You might also be interested in these eBooks

Info:

Periodical:

Materials Science Forum (Volumes 527-529)

Pages:

1469-1472

Citation:

Online since:

October 2006

Export:

Price:

Permissions CCC:

Permissions PLS:

Сopyright:

© 2006 Trans Tech Publications Ltd. All Rights Reserved

Share:

Citation:

[1] F. H. Ruddy, et al.: IEEE Trans. Nucl. Sci., Vol. 45 (1998), pp.536-539.

Google Scholar

[2] M. Rogalla et al.: Nucl. Phys. B (Proc. Suppl. ), Vol. 78 (1999), p.516.

Google Scholar

[3] W. Cunningham et al.: Nucl. Instrum. Methods, Vol. A487 (2002), pp.33-39.

Google Scholar

[4] F. Nava, P. Vanni, C. Lanzieri, and C. Canali: Nucl. Instrum. Methods Phys. Res., Vol. A437 (1999), pp.354-358.

Google Scholar

[5] M. Bruzzi, F. Nava, S. Russo, S. Sciortino, and P. Vanni: Diamond Relat. Mater., Vol. 10 (2001), pp.657-661.

Google Scholar

[6] F. Nava et al.: Mater. Sci. Forum, Vol. 353-356 (2000), pp.757-762.

Google Scholar

[7] G. Bertuccio, R. Casiraghi, and F. Nava: IEEE Trans. Nucl. Sci., Vol. 48 (2001), pp.232-236.

Google Scholar

[8] F. Nava et al.: Nucl. Instrum. Methods Phys. Res. A, Vol. 505 (2003), pp.645-655.

Google Scholar

[9] F. Nava et al.: IEEE Trans. Nucl. Sci., Vol. 51 (2004), pp.238-244.

Google Scholar

[10] RD50, LHCC 2002-2003, 15 February 2002, CERN, Geneva.

Google Scholar

[11] F. Gao, et el.: Nucl. Instr. & Meth. in Phys. Res. B 191 (2002), pp.487-496.

Google Scholar

[12] S. Sciortino et. al.: Nucl. Instrum. Methods Phys. Res. A, Vol. 552 (2005), pp.138-145.

Google Scholar

[13] A. S. Grove, Physics and Technology of Semiconductor Devices (John Wiley and Sons, 1967). -2000 0 2000 4000 6000 0 2000 4000 6000 8000 10000 Counts Channel [e] 55 V 110 V 220 V 330 V 385 V Fig. 5: Pulse height spectrum of the collected charge signal at different voltages for the diode with D = 1 mm. At 250 V the signal saturates.

Google Scholar