In semiconductor physics, the Haynes–Shockley experiment was an experiment that demonstrated that diffusion of minority carriers in a semiconductor could result in a current. The experiment was reported in a short paper by Haynes and Shockley in 1948,[1] with a more detailed version published by Shockley, Pearson, and Haynes in 1949.[2][3] The experiment can be used to measure carrier mobility, carrier lifetime, and diffusion coefficient.
In the experiment, a piece of semiconductor gets a pulse of holes, for example, as induced by voltage or a short laser pulse.
Equations
To see the effect, we consider a n-type semiconductor with the length d. We are interested in determining the mobility of the carriers, diffusion constant and relaxation time. In the following, we reduce the problem to one dimension.
The equations for electron and hole currents are:
\( j_{e}=+\mu _{n}nE+D_{n}{\frac {\partial n}{\partial x}} \)
\( j_{p}=+\mu _{p}pE-D_{p}{\frac {\partial p}{\partial x}} \)
where the js are the current densities of electrons (e) and holes (p), the μs the charge carrier mobilities, E is the electric field, n and p the number densities of charge carriers, the Ds are diffusion coefficients, and x is position. The first term of the equations is the drift current, and the second term is the diffusion current.
Derivation
We consider the continuity equation:
\( {\displaystyle {\frac {\partial n}{\partial t}}={\frac {-(n-n_{0})}{\tau _{n}}}+{\frac {\partial j_{e}}{\partial x}}} \)
\( {\frac {\partial p}{\partial t}}={\frac {-(p-p_{0})}{\tau _{p}}}-{\frac {\partial j_{p}}{\partial x}} \)
Subscript 0s indicate equilibrium concentrations. The electrons and the holes recombine with the carrier lifetime τ.
We define
\( } p_{1}=p-p_{0}\,,\quad n_{1}=n-n_{0} \)
so the upper equations can be rewritten as:
\( {\frac {\partial p_{1}}{\partial t}}=D_{p}{\frac {\partial ^{2}p_{1}}{\partial x^{2}}}-\mu _{p}p{\frac {\partial E}{\partial x}}-\mu _{p}E{\frac {\partial p_{1}}{\partial x}}-{\frac {p_{1}}{\tau _{p}}} \)
\( {\frac {\partial n_{1}}{\partial t}}=D_{n}{\frac {\partial ^{2}n_{1}}{\partial x^{2}}}+\mu _{n}n{\frac {\partial E}{\partial x}}+\mu _{n}E{\frac {\partial n_{1}}{\partial x}}-{\frac {n_{1}}{\tau _{n}}} \)
In a simple approximation, we can consider the electric field to be constant between the left and right electrodes and neglect ∂E/∂x. However, as electrons and holes diffuse at different speeds, the material has a local electric charge, inducing an inhomogeneous electric field which can be calculated with Gauss's law:
\( {\frac {\partial E}{\partial x}}={\frac {\rho }{\epsilon \epsilon _{0}}}={\frac {e_{0}((p-p_{0})-(n-n_{0}))}{\epsilon \epsilon _{0}}}={\frac {e_{0}(p_{1}-n_{1})}{\epsilon \epsilon _{0}}} \)
where ε is permittivity, ε0 the permittivity of free space, ρ is charge density, and e0 elementary charge.
Next, change variables by the substitutions:
\( p_{1}=n_{{\text{mean}}}+\delta \,,\quad n_{1}=n_{{\text{mean}}}-\delta \,, \)
and suppose δ to be much smaller than n mean {\displaystyle n_{\text{mean}}} n_{{\text{mean}}}. The two initial equations write:
\( {\frac {\partial n_{{\text{mean}}}}{\partial t}}=D_{p}{\frac {\partial ^{2}n_{{\text{mean}}}}{\partial x^{2}}}-\mu _{p}p{\frac {\partial E}{\partial x}}-\mu _{p}E{\frac {\partial n_{{\text{mean}}}}{\partial x}}-{\frac {n_{{\text{mean}}}}{\tau _{p}}} \)
\( {\frac {\partial n_{{\text{mean}}}}{\partial t}}=D_{n}{\frac {\partial ^{2}n_{{\text{mean}}}}{\partial x^{2}}}+\mu _{n}n{\frac {\partial E}{\partial x}}+\mu _{n}E{\frac {\partial n_{{\text{mean}}}}{\partial x}}-{\frac {n_{{\text{mean}}}}{\tau _{n}}} \)
Using the Einstein relation \( \mu =e\beta D \), where β is the inverse of the product of temperature and the Boltzmann constant, these two equations can be combined:
\( {\frac {\partial n_{{\text{mean}}}}{\partial t}}=D^{*}{\frac {\partial ^{2}n_{{\text{mean}}}}{\partial x^{2}}}-\mu ^{*}E{\frac {\partial n_{{\text{mean}}}}{\partial x}}-{\frac {n_{{\text{mean}}}}{\tau ^{*}}}, \)
where for D*, μ* and τ* holds:
\( D^{*}={\frac {D_{n}D_{p}(n+p)}{pD_{p}+nD_{n}}} \), \( \mu ^{*}={\frac {\mu _{n}\mu _{p}(n-p)}{p\mu _{p}+n\mu _{n}}} \) and \( {\frac {1}{\tau ^{*}}}={\frac {p\mu _{p}\tau _{p}+n\mu _{n}\tau _{n}}{\tau _{p}\tau _{n}(p\mu _{p}+n\mu _{n})}}. \)
Considering n >> p or p → 0 (that is a fair approximation for a semiconductor with only few holes injected), we see that D* → Dp, μ* → μp and 1/τ* → 1/τp. The semiconductor behaves as if there were only holes traveling in it.
The final equation for the carriers is:
\( n_{{\text{mean}}}(x,t)=A{\frac {1}{{\sqrt {4\pi D^{*}t}}}}e^{{-t/\tau ^{*}}}e^{{-{\frac {(x+\mu ^{*}Et-x_{0})^{2}}{4D^{*}t}}}} \)
This can be interpreted as a Dirac delta function that is created immediately after the pulse. Holes then start to travel towards the electrode where we detect them. The signal then is Gaussian curve shaped.
Parameters μ, D and τ can be obtained from the shape of the signal.
\( \mu ^{*}={\frac {d}{Et_{0}}} \)
\( D^{*}=(\mu ^{*}E)^{2}{\frac {(\delta t)^{2}}{16t_{0}}} \)
where d is the distance drifted in time t0, and δt the pulse width.
See also
Alternating current
Conduction band
Convection–diffusion equation
Direct current
Drift current
Free electron model
Random walk
References
Haynes, J.; Shockley, W. (1949). "Investigation of Hole Injection in Transistor Action". Physical Review. 75 (4): 691. Bibcode:1949PhRv...75..691H. doi:10.1103/PhysRev.75.691.
Shockley, W. and Pearson, G. L., and Haynes, J. R. (1949). "Hole injection in germanium – Quantitative studies and filamentary transistors". Bell System Technical Journal. 28: 344–366. doi:10.1002/j.1538-7305.1949.tb03641.x.
Jerrold H. Krenz (2000). Electronic concepts: an introduction. Cambridge University Press. p. 137. ISBN 978-0-521-66282-6.
Hellenica World - Scientific Library
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