The temperature dependence performance of ultraviolet radiation detectors T. V. Blank, Yu. A. Goldberg, O. V. Konstantinov Ioffe Physico-Technical Institute of Russian Academy of Science, St. Petersburg, Russia IWORID 2002 AMSTERDAM - PowerPoint PPT Presentation

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The temperature dependence performance of ultraviolet radiation detectors T. V. Blank, Yu. A. Goldberg, O. V. Konstantinov Ioffe Physico-Technical Institute of Russian Academy of Science, St. Petersburg, Russia IWORID 2002 AMSTERDAM

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Title: The temperature dependence performance of ultraviolet radiation detectors T. V. Blank, Yu. A. Goldberg, O. V. Konstantinov Ioffe Physico-Technical Institute of Russian Academy of Science, St. Petersburg, Russia IWORID 2002 AMSTERDAM


1
The temperature dependence performance of
ultraviolet radiation detectorsT. V. Blank, Yu.
A. Goldberg, O. V. KonstantinovIoffe
Physico-Technical Instituteof Russian Academy of
Science,St. Petersburg, RussiaIWORID 2002
AMSTERDAM
2
Outline
Aim
  • Determination of
  • photoelectric conversion process mechanism in
    Schottky photodetectors
  • temperature stability of UV detectors
  • The temperature dependence of the quantum
    efficiency of GaP Schottky photodetectors.
  • The fluctuation traps model.
  • Comparison of the temperature dependencies of the
    quantum efficiency in Schottky and p-n
    photodetectors based on GaAs.
  • The temperature dependence of the quantum
    efficiency of Si Schottky photodetectors.
  • The temperature dependence of the quantum
    efficiency of 4H-SiC Schottky photodetectors.
  • Conclusion.

3
Experimental procedure
  • where ? - quantum efficiency
  • I - photocurrent
  • ? - incident light power
  • h? - photon energy
  • q - electron charge

4
The temperature dependence of the quantum
efficiency of GaP Schottky photodetectors
The quantum efficiency ? of GaP Schottky
photodetectors as a function of the temperature
for several photon energies.
  • The spectrum of the quantum efficiency ? of GaP
    Schottky photodetectors at 300 K.

5
Optical losses
Bulk losses
where R is reflection coefficient ? is
dielectric constant
Others losses
The effective optical length Ln of GaP as a
function of the photon energy, 300 K, W is the
width of the space-change region.
  • surface recombination
  • thermionic emission of thermalized and hot
    photoelectrons in the metal

6
The fluctuation traps model
  • ?(1-R)?(1-?hot)(1-?th?rm)
  • 1-?th?rm?-??/kT
  • ?1
  • ?(1-R)(1-?hot)?-??/kT,
  • where
  • ? - quantum efficiency,
  • R - reflection coefficient
  • ? - internal quantum yield
  • ?hot - loss factor of hot photocarriers
  • ?th?rm - loss factor of thermalized photocarriers
  • ?? - activation energy of the localized
    photocarriers
  • k - Boltzmanns constant
  • ? - temperature


7
Schottky and p-n photodetectors based on GaAs
The spectrum of the quantum efficiency ? of
GaAs p-n photodetectors at 300 K.
The spectrum of the quantum efficiency ? of
GaAs Schottky photodetectors at 300 K.
8
Comparison of the temperature dependencies of the
quantum efficiency in Schottky and p-n
photodetectors based on GaAs
The quantum efficiency ? of GaAs p-n
photodetectors as a function of the temperature
for several photon energies.
The quantum efficiency ? of GaAs Schottky
photodetectors as a function of the temperature
for several photon energies.
9
The temperature dependence of the quantum
efficiency of p-n photodetectors based on Si
The spectrum of the quantum efficiency ? of Si
p-n photodetectors at 300 K
The quantum efficiency ? of Si p-n
photodetectors as a function of the temperature
for several photon energies.
10
4H-SiC Schottky photodetectors
  • The spectrum of the quantum efficiency ? of
    4H-SiC Schottky photodetectors at 300 K (line 1)
    and the spectrum of the relative effectiveness of
    different photon energies in bactericidal
    ultraviolet radiation (line 2).

11
The temperature dependence of the quantum
efficiency of 4H-SiC Schottky photodetectors
At 300K W0.3 ?m Lh1.4 ?m L?thWoLh?1.7
?m??L?-1?hn4.5 eV where L? is effective
optical absorption length L?th is threshold
effective optical absorption length W is width of
the space-change region Lh is hole diffusion
length ? is absorption coefficient
12
The photoelectric conversion mechanism in 4H-SiC
Schottky photodetectors
Band structure of 4H-SiC and scheme of different
optical transitions.
13
Conclusion
  • For Schottky photodetectors (based on GaAs, GaP,
    4H-SiC) the quantum efficiency increases with
    temperature for all photon energies.
  • For p-n photodetectors based on GaAs and Si the
    quantum efficiency is temperature independent in
    the region of intrinsic absorption.
  • Near-surface imperfections manifest themselves as
    the fluctuation traps and have an influence on
    the photoelectric conversion process in Schottky
    photodetectors.

Future
  • The temperature dependence of the quantum
    efficiency of p-n and Schottky photodetectors
    based on GaN.
  • The temperature dependence of the quantum
    efficiency of not deep p-n photodetectors (based
    on 4H-SiC).
  • External electric field Influence on the quantum
    efficiency for UV photodetectors.
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