Impurity band density of states in the atomic limit

1980 ◽  
Vol 58 (8) ◽  
pp. 1142-1150 ◽  
Author(s):  
K. L. Liu ◽  
B. Bergersen ◽  
P. Modrak

Model calculations are presented for the density of states in the impurity band of a semiconductor. The calculations are based on the Hubbard model in the atomic (i.e., infinite U) limit and are thus appropriate to impurity concentration below the critical one for the metal–insulator transition. No ordering of the electron spin is assumed, instead all spin configurations are taken to be equally probable. The impurity distribution is taken to be random. Calculations are carried out with a Gaussian overlap integral as a function of impurity–impurity distance and with the transfer integral obtained from hydrogenic wave function. The first seven moments of the density of states distribution of the Gaussian model and the first six moments of the hydrogenic model are calculated using a diagrammatic method. We also discuss asymptotic expressions for the distribution in the high and low density limits. Intepolation methods to reconstruct the distribution from the moments are investigated. It is believed that the methods used are suitable for generalizations to more realistic model Hamiltonians.

1982 ◽  
Vol 60 (12) ◽  
pp. 1743-1750 ◽  
Author(s):  
K. L. Liu ◽  
P. Modrak ◽  
B. Bergersen

A marked magnetic field dependence is found for the impurity band density of states in an idealized model of a doped semiconductor. The calculations are based on the Hubbard model in the atomic limit. We have obtained exactly the first eight moments of the distribution using a Gaussian model for the hopping integral, and the first seven moments with a hydrogenic model. A simple Zeeman type response of the spin system to the magnetic field is assumed. The predicted density of states is then obtained using a modified moment method with a trial density of states function obtained from the expected asymptotic behaviour of the distribution. Finally, we adjust the parameters of our models to correspond to phosphorous doped silicon below the metal insulator transition.


1973 ◽  
Vol 45 (4) ◽  
pp. 331-332 ◽  
Author(s):  
W. Brenig ◽  
K. Schönhammer

1996 ◽  
Vol 69 (1) ◽  
pp. 81-91 ◽  
Author(s):  
R. Ding ◽  
A. I. Leonov ◽  
A. Y. Coran

Abstract Vulcanization kinetics for a SBR compound was studied by using both curemeter and DSC methods by a kinetic approach. A simplified but realistic model reaction scheme was used to simulate both induction and curing periods simultaneously. Model parameters were extracted from isothermal curemeter experiments. The model prediction demonstrated a good agreement with isothermal curemeter data over a temperature range of 120°C to 180°C. The variation of equilibrium modulus with temperature, observed from cure curves, can also be predicted. However, DSC experiments showed a different reaction behavior in the curing period as compared to model calculations. This was explained by the assumption that the reaction heat observed in DSC is due to all possible exothermal reactions, and the formation of crosslinks is only a part of these reactions. Hence, the curemeter can provide a good indication of crosslink formation, while DSC displays the entire reaction heat released during the vulcanization process. The kinetic approach allows one to incorporate vulcanization kinetics into the practical simulation of reactive processing operations.


2006 ◽  
Vol 38 (02) ◽  
pp. 430-450 ◽  
Author(s):  
Georg Lindgren

Gaussian wave models have been successfully used since the early 1950s to describe the development of random sea waves, particularly as input to dynamic simulation of the safety of ships and offshore structures. A drawback of the Gaussian model is that it produces stochastically symmetric waves, which is an unrealistic feature and can lead to unconservative safety estimates. The Gaussian model describes the height of the sea surface at each point as a function of time and space. The Lagrange wave model describes the horizontal and vertical movements of individual water particles as functions of time and original location. This model is physically based, and a stochastic version has recently been advocated as a realistic model for asymmetric water waves. Since the stochastic Lagrange model treats both the vertical and the horizontal movements as Gaussian processes, it can be analysed using methods from the Gaussian theory. In this paper we present an analysis of the stochastic properties of the first-order stochastic Lagrange waves model, both as functions of time and as functions of space. A Slepian model for the description of the random shape of individual waves is also presented and analysed.


1992 ◽  
Vol 06 (29) ◽  
pp. 1881-1885
Author(s):  
I.C. DA CUNHA LIMA ◽  
A. FERREIRA DA SILVA

Quasi-one-dimensional channels have already been fabricated by holographic lithography on semiconductor heterostructures. We study the formation of an impurity band for shallow donors located inside the channels assuming they have been created by applying a modulated gate voltage in a quantum well of AlxGa1−xAs−GaAs. We calculate the changes in the impurity density of states as a function of the gate voltage. It is shown that the increase of the applied gate voltage leads to higher binding energy and larger impurity bandwidth.


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