1958
DOI: 10.1063/1.1723358
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Space Charge Calculations for Semiconductors

Abstract: The electric field at the surface of a semiconductor is obtained as a function of the semiconductor bulk properties and the potential difference across the space charge region. The treatment is general enough to take into account degenerate free carrier distributions and partial ionization of impurities, either in the neutral bulk or the space charge region, or both. A one-dimensional model with a spacially homogeneous impurity distribution is assumed. The density of states in the conduction and valence bands … Show more

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Cited by 210 publications
(65 citation statements)
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“…The last assumption introduces errors of about 20%, see for example refs. [23,24]. Then it follows that the band bending is at least -340 mV (uncertainty about 10 mV), in good accordance with Margoninski et al 120,211.…”
Section: Resultssupporting
confidence: 75%
“…The last assumption introduces errors of about 20%, see for example refs. [23,24]. Then it follows that the band bending is at least -340 mV (uncertainty about 10 mV), in good accordance with Margoninski et al 120,211.…”
Section: Resultssupporting
confidence: 75%
“…The surface is considered to be nondegenerate, no fast holes and fast electrons are assumed, AN is neglected, the sample is considered intrinsic, and #ps is replaced by the known value #p. The last assumption introduces errors of about 20%, see for example refs. [21,25]. Then it follows that the value is at least -280 mV (uncertainty about 10 mV), in good accordance with Boonstra et at.…”
supporting
confidence: 76%
“…The charges induce electric fields at the surface that cause band bending. The electric field at the surface may be formally described by the solution of the Poisson equation for a dimensionless potential kT V e o ≡ ν [36,37]:…”
Section: Surface Charged Statesmentioning
confidence: 99%