Technology developments and first measurements of Low Gain Avalanche Detectors (LGAD) for high energy physics applications

Abstract This paper introduces a new concept of silicon radiation detector with intrinsic multiplication of the charge, called Low Gain Avalanche Detector (LGAD). These new devices are based on the standard Avalanche Photo Diodes (APD) normally used for optical and X-ray detection applications. The main differences to standard APD detectors are the low gain requested to detect high energy charged particles, and the possibility to have fine segmentation pitches: this allows fabrication of microstrip or pixel devices which do not suffer from the limitations normally found [1] in avalanche detectors. In addition, a moderate multiplication value will allow the fabrication of thinner devices with the same output signal of standard thick substrates. The investigation of these detectors provides important indications on the ability of such modified electrode geometry to control and optimize the charge multiplication effect, in order to fully recover the collection efficiency of heavily irradiated silicon detectors, at reasonable bias voltage, compatible with the voltage feed limitation of the CERN High Luminosity Large Hadron Collider (HL-LHC) experiments [2] . For instance, the inner most pixel detector layers of the ATLAS tracker will be exposed to fluences up to 2×10 16  1 MeV n eq /cm 2 , while for the inner strip detector region fluences of 1×10 15  n eq /cm 2 are expected. The gain implemented in the non-irradiated devices must retain some effect also after irradiation, with a higher multiplication factor with respect to standard structures, in order to be used in harsh environments such those expected at collider experiments.

[1]  L. Rossi,et al.  High Luminosity Large Hadron Collider : A description for the European Strategy Preparatory Group , 2012 .

[2]  C. R. Crowell,et al.  Threshold energy effect on avalanche breakdown voltage in semiconductor junctions , 1975 .

[3]  G. Entine,et al.  Radiation detection performance of very high gain avalanche photodiodes , 1994 .

[4]  Nicholas A. Lockerbie,et al.  Nuclear Instruments and Methods in Physics Research A , 2014 .

[5]  P. Cochat,et al.  Et al , 2008, Archives de pediatrie : organe officiel de la Societe francaise de pediatrie.

[6]  G. Lutz,et al.  Semiconductor Radiation Detectors , 2007 .

[7]  P. Allport,et al.  Enhanced efficiency of segmented silicon detectors of different thicknesses after proton irradiations up to 1×1016 neq cm2 , 2010 .

[8]  B. Jayant Baliga,et al.  Fundamentals of Power Semiconductor Devices , 2008 .

[9]  V. Cindro,et al.  Comparison of pad detectors produced on different silicon materials after irradiation with neutrons, protons and pions ☆ , 2010 .

[10]  Mara Bruzzi,et al.  Radiation damage in silicon detectors for high-energy physics experiments , 2001 .

[11]  R. Gilmore,et al.  Avalanche Photodiodes as Proportional Particle Detectors , 1997 .

[12]  V. Cindro,et al.  Observation of full charge collection efficiency in heavily irradiated n+p strip detectors irradiated up to 3×1015 neq/cm2 , 2010 .

[13]  C. R. Crowell,et al.  Temperature dependence of avalanche multiplication in semiconductors , 1966 .