1985
DOI: 10.1063/1.334822
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Nonlinear transient response of extrinsic Ge far-infrared photoconductors

Abstract: Physical mechanisms responsible for nonlinear phenomena and anomalous transient response of cooled extrinsic far-infrared photoconductors are discussed. A simple model describing carrier generation, trapping, and impact ionization is presented, which describes the transient response on fast time scales 10−3 to 10−4 sec, neglecting changes in space charge. Carrier heating by a dc electric field produces relatively fast, damped oscillatory response to external excitation. A small-signal analysis of these equatio… Show more

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Cited by 92 publications
(39 citation statements)
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“…The transport coefficients V , K and R are, respectively, the average (drift) velocity of microscopic charge carriers (holes in the case of p-Ge), and coefficients describing the creation of free carriers via impurity impact ionization and the destruction of free carriers by capture onto an available impurity trapping site (i.e., neutral acceptor). All are nonlinear functions of electric field, and their forms and plots have been discussed extensively in the literature [5,13,14]. In this paper we use the same forms as in Ref.…”
Section: The Reduced Drift-diffusion Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…The transport coefficients V , K and R are, respectively, the average (drift) velocity of microscopic charge carriers (holes in the case of p-Ge), and coefficients describing the creation of free carriers via impurity impact ionization and the destruction of free carriers by capture onto an available impurity trapping site (i.e., neutral acceptor). All are nonlinear functions of electric field, and their forms and plots have been discussed extensively in the literature [5,13,14]. In this paper we use the same forms as in Ref.…”
Section: The Reduced Drift-diffusion Modelmentioning
confidence: 99%
“…Many of these phenomena have been successfully explained by means of a drift-diffusion model which includes impurity trapping of mobile holes and impact ionization of neutral acceptors [6,13]. Although much work has been done on this model problem (see [14] and references therein), important basic questions concerning its asymptotic description and chaos under time independent voltage bias are still open.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, however, some attempts have been made to solve the differential equations describing steady state carrier transport, including the boundary condition for an ideal ohmic contact (52). The equations governing the physics of the near-contact region will be reviewed and a summary of the steady state solution will be given.…”
Section: Contact Modelingmentioning
confidence: 99%
“…6 The photoconductive gain in turn is given by G =-'rr= Ir (Eb)X (lb) where T tr is the mean time for carriers to transit the interelectrode distance 1, A is the drift mobility, and Eb is the dc bias field on the detector. Thus there are three fundamental material parameters that completely characterize such a detector: mobility; recombination time; and quantum efficiency.…”
Section: Introductionmentioning
confidence: 99%