state of the art on epitaxial gaas detectors

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1 State of the art on epitaxial GaAs detectors G.C. Sun a , N. Mañez a , M. Zazoui a , A.Al-Ajili b , V.O'Shea b , F.Quarati b , K.M.Smith b , D. Chambellan c , O. Gal c , Ph. Pillot c , M. Lenoir d , J. P. Montagne d , A. Bchetnia e , J.C. Bourgoin f a LMDH, Université Pierre et Marie Curie (Paris 6), France b Department of Physics and Astronomy, University of Glasgow,UK. c LIST/DIMRI, CEA , France d Hospital Armand Trousseau, Paris, France. e Lab. de Physique des Matériaux, Faculté des Sciences de Monastir, Tunisie f GESEC R&D, 68 Avenue de la Forêt, 77210 Avon, France GESEC R&D Inc. Semiconductor Materials Engineering

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GESEC R&D Inc. Semiconductor Materials Engineering. State of the art on epitaxial GaAs detectors. - PowerPoint PPT Presentation

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Page 1: State of the art on epitaxial GaAs detectors

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State of the art on epitaxial GaAs detectors G.C. Suna, N. Mañeza, M. Zazouia, A.Al-Ajilib, V.O'Sheab, F.Quaratib,

K.M.Smithb, D. Chambellanc, O. Galc, Ph. Pillotc, M. Lenoird, J. P. Montagned,

A. Bchetniae, J.C. Bourgoinf

a LMDH, Université Pierre et Marie Curie (Paris 6), Franceb Department of Physics and Astronomy, University of Glasgow,UK.c LIST/DIMRI, CEA , Franced Hospital Armand Trousseau, Paris, France.e Lab. de Physique des Matériaux, Faculté des Sciences de Monastir, Tunisief GESEC R&D, 68 Avenue de la Forêt, 77210 Avon, France

GESEC R&D Inc.Semiconductor Materials Engineering

Page 2: State of the art on epitaxial GaAs detectors

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Motivation

Decrease the dose (more than a factor of 10 compared to scintillator flat panels) in X-ray imaging

Page 3: State of the art on epitaxial GaAs detectors

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Outline

Review of X-ray detection with GaAs

Development of epi-growth of GaAs

Device processing

Device electrical characteristics

Performance of radiation detectors

Limitations of current devices and ways to overcome

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History of GaAs radiation detectors (1)

Early work with LPE GaAs

(by Tavendale group, 1970)

Three typical 241Am and 57Co -ray spectra, at 100V bias and 130K, from 1.5mm diameter, 80m thick LPE GaAs surface barrier detectors, (carrier concentration ~ 6 x 1013 cm-

3), fabricated on tin-doped substrates.

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History of GaAs radiation detectors (2)MBE epi-GaAs

(Bertuccio et al., 1996/97)

Pulse height spectrum of photons from an 241Am source detected in a 170 x 320m2 , 5 micron thick MBE undoped GaAs diode detector at 15V reverse bias

Page 6: State of the art on epitaxial GaAs detectors

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Progress in the growth of epitaxial GaAs

• One 4 inch, 550 µm layer • Thickness profile of epi-GaAs grown on four inch substrate

Source: SI GaAsn+ substrate: n type (<1014 cm-3)

SI substrate: p type (<1014 cm-3)

Page 7: State of the art on epitaxial GaAs detectors

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Electronic properties of epitaxial GaAs

• Photoluminescence mapping

SI GaAs Epitaxial GaAs layer CdTe

Page 8: State of the art on epitaxial GaAs detectors

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Technique to fabricate detectors

ohmic contact

p+ ion implantation (35 nm)

GaAs epilayer

n+ substrate (Cz GaAs)

n+ ion implantation (35 nm)

Page 9: State of the art on epitaxial GaAs detectors

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Current-Voltage characteristic of a small pad diode

2 nA/mm2 at 50 V

Page 10: State of the art on epitaxial GaAs detectors

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Alpha particle pulse height spectra

• Combined source 241Am(5.5 MeV), 244Cm (5.8 MeV) and 239Pu (5.2 MeV)

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Charge collection efficiency

Fitted values at 100 V, giving charge collection efficiency of 85%.

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Pulse height spectra of monoenergetic X-rays

• Characteristic K-series X-rays of Ag, Ba and Nb.

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Photocurrent versus radiation dose

1mm2 epitaxial GaAs diode detector

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Limitation: width of depleted zone

Three ways to overcome it:

1. growth conditions

2. electron irradiation

3. use of 3D detectors

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1 MeV electron irradiation

Low defects not enough to compensate free carriers. Irradiation introduces defects increase depleted depth

Before

irradiation

After

irradiation

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3D detectors

‘3D’ SI-LEC GaAs pixel detector bonded to DASH-E ROIC

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End