Physics and Engineering of Radiation Detection

(Martin Jones) #1

5.1. Semiconductor Detectors 281


Eg= 1.42 eV


EX= 1.90 eV


EL= 1.71 eV


Wavevector


Holes


Energy


<100> <111>

Figure 5.1.20: Band structure diagram of gallium arsenide showing
energy versus wavenumber (reproduced from (47)). The subscripts of
Erepresent different energy levels. The number in brackets (100 and
111) are the Miller indices. A Miller index represents the orientation
of an atomic plane in a crystal lattice.

T (K)

250 260 270 280 290 300 310

(eV)g
E

1.42

1.425

1.43

1.435

1.44

1.445

Figure 5.1.21: Variation of gal-
lium arsenide band gap energy
with absolute temperature.

valence bands inGaAscan be written as (47)


Nc=8. 63 × 1013 T^3 /^2

[

1 − 1. 93 × 10 −^4 T− 4. 19 × 10 −^8 T^2

+21exp

(


EL

2 kBT

)

+44exp

(


EX

2 kBT

)]

(5.1.46)

and
Nv=1. 83 × 1015 T^3 /^2 , (5.1.47)

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