This contribution presents a parametric analysis and TCAD simulations of the radiation resistance of compensated LGADs. In such designs, the gain layer is engineered through compensation of acceptor and donor dopants. Following radiation-induced deactivation of donor and acceptor atoms in the gain layer, the goal is to preserve the multiplication mechanism beyond the radiation tolerance of current LGAD technology of 2 & times;10(15) n(eq)/cm(2) for 50 mu m-thick sensors. The conditions under which compensated LGADs may achieve improved radiation hardness with respect to conventional LGAD technology are presented. Starting from assumptions regarding acceptor and donor deactivation rates, the optimal initial concentrations that maximize the extent of LGAD radiation tolerance is computed. If, as preliminary observations suggest, the donor removal rate exceeds that of the acceptor, compensated LGADs would need to be designed to operate initially under a high external bias close to the single-event burnout limit.

How to operate a compensated LGAD

S. Galletto
First
;
A. R. Altamura;M. Durando;L. Massaccesi;M. Tornago;V. Sola
2026-01-01

Abstract

This contribution presents a parametric analysis and TCAD simulations of the radiation resistance of compensated LGADs. In such designs, the gain layer is engineered through compensation of acceptor and donor dopants. Following radiation-induced deactivation of donor and acceptor atoms in the gain layer, the goal is to preserve the multiplication mechanism beyond the radiation tolerance of current LGAD technology of 2 & times;10(15) n(eq)/cm(2) for 50 mu m-thick sensors. The conditions under which compensated LGADs may achieve improved radiation hardness with respect to conventional LGAD technology are presented. Starting from assumptions regarding acceptor and donor deactivation rates, the optimal initial concentrations that maximize the extent of LGAD radiation tolerance is computed. If, as preliminary observations suggest, the donor removal rate exceeds that of the acceptor, compensated LGADs would need to be designed to operate initially under a high external bias close to the single-event burnout limit.
2026
TREDI
Perugia
Feb 17 – 19, 2026
21
08
C08012
C08021
Detector modelling and simulations II (electric fields, charge transport, multiplication and induction, pulse formation, electron emission, etc); Radiation-hard detectors; Solid state detectors
S. Galletto; N. Cartiglia; A.R. Altamura; R. Arcidiacono; A. Bisht; M. Centis Vignali; T. Croci; M. Durando; M. Ferrero; A. Fondacci; L. Massaccesi; A...espandi
File in questo prodotto:
File Dimensione Formato  
Galletto_2026_J._Inst._21_C08012.pdf

Accesso aperto

Tipo di file: PDF EDITORIALE
Dimensione 1.14 MB
Formato Adobe PDF
1.14 MB Adobe PDF Visualizza/Apri

I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.

Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/2165910
Citazioni
  • ???jsp.display-item.citation.pmc??? ND
  • Scopus ND
  • ???jsp.display-item.citation.isi??? 0
social impact