The microscopic physics, device physics, and system performance of quantum
well infrared photodetectors (QWIPs) are reviewed. QWIPs which respond to n
ormally incident radiation without the need for an optical grating are of p
articular interest because they can be fabricated with fewer process steps.
Recent demonstrations of n-type QWIPs (n-QWIPs) which show a significant d
etectivity of 4 x 10(10) cm root Hz/W without the use of an optical grating
are discussed here. This detectivity is significant because it is large en
ough for focal plane array (FPA) performance to be limited by the uniformit
y of processing rather than the size of the single pixel detectivity. Studi
es of the microscopic physics of quantum wells are summarized to elucidate
the physical origin of the intersubband absorption of normally incident rad
iation. The selection rules for intersubband absorption by holes in a p-dop
ed QWIP (p-QWIP) and electrons in an n-QWIP are reviewed. In particular, it
is shown that the hole intersubband absorption is typically weaker than bo
th the conduction intersubband absorption and the valence band-to-conductio
n band absorption. It is also shown that uniaxial strain does not have a la
rge effect on the strength or the selection rules of intersubband absorptio
n because the Hamiltonian describing uniaxial strain has the same (tetragon
al) symmetry as that describing the confinement of carriers in the quantum
wells along the growth direction. Also reviewed are device models which yie
ld analytical expressions for the number of, and the distance over which, c
arriers are depleted from quantum wells under conditions of insufficient ca
rrier injection. This carrier depletion becomes important when the incident
photon flux is large or when the QWIP operating temperature is low. Unifor
mity of QWIP device parameters is important in determining the ultimate arr
ay signal-to-noise ratio (SNR). Examples of high-resolution X-ray diffracti
on methods used to find the layer width variations of QWIPs grown by molecu
lar beam epitaxy are reviewed. The spread of the measured full-width at hal
f-maxima (FWHM) of superlattice diffraction peaks with the diffraction orde
r was used with Bragg's Law to obtain the measured layer width variation in
the growth direction. A theoretical study of different noise mechanisms wh
ich contribute to QWIP performance was carried out. A key result is that, w
hen the SNR is limited by either fixed pattern noise or thermal leakage arr
ival noise, the largest expected QWIP SNR occurs when the number of quantum
wells in the QWIP is at the optimal value of about eta(1)(-1), where n(1)
is the quantum efficiency of a QWIP having only one quantum well. Common QW
IP designs used in industry are evaluated. In particular, different physica
l models for the leakage (sequential tunneling, thermionic and thermionic f
ield assisted leakage) are reviewed. A new result is a physical model, deri
ved from the Kronig-Penney model, for the tunneling leakage in existing QWI
P designs in which the confinement barrier is a semiconductor superlattice.
The tunneling leakage in such QWIPs is shown to vary exponentially with th
e average (rather than the full) height of the superlattice barrier. (C) 20
00 Elsevier Science S.A. All rights reserved.