Apparent Density of Thin Evaporated Films
Measurements of the apparent densities of copper and silver films formed by evaporation are described. The interpretation of the results and the manifestations of low apparant densities in physical ex...
Measurements of the apparent densities of copper and silver films formed by evaporation are described. The interpretation of the results and the manifestations of low apparant densities in physical ex...
Radiation Damage Effects on Order-Disorder in Nickel-Manganese Alloys
Effects of fast neutron irradiation in a nuclear reactor on order-disorder in a series of nickel-manganese alloys ranging from 16.5 to 31.9 atomic percent manganese have been studied by resistivity an...
Effects of fast neutron irradiation in a nuclear reactor on order-disorder in a series of nickel-manganese alloys ranging from 16.5 to 31.9 atomic percent manganese have been studied by resistivity an...
Noise in Semiconductors: Spectrum of a Two-Parameter Random Signal
J. Appl. Phys. 25, 341 (1954); doi:10.1063/1.1721637
Issue Date: March 1954
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With intended application to the theory of current noise in semiconductors, the spectrum is calculated of a random signal which may be in one of two states (YES-NO: random telegraph signal), where the mean lives 
and 
of the two states may be different. The form of the spectrum is the same as for the case with equal lives, the single parameter for that (classical) case now being replaced by 2[(1/)+(1/)]−1; i.e., the rates of transition are additive.
Journal of Applied Physics is copyrighted by The American Institute of Physics.
and of the two states may be different. The form of the spectrum is the same as for the case with equal lives, the single parameter for that (classical) case now being replaced by 2[(1/)+(1/)]−1; i.e., the rates of transition are additive.
Journal of Applied Physics is copyrighted by The American Institute of Physics.
| History: | Received July 15, 1953 |
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http://link.aip.org/link/?JAPIAU/25/341/1 |
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REFERENCES (4)
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- S. O. Rice, Bell System Tech. J. 23, 282 (1945), Sec. 2.7.
- This has the form of the expression obtained by J. Bernamont,
Proc. Phys. Soc. (London) 49, E138 (1937) . - A. Van der Ziel, J. Appl. Phys. 24, 222 (1953);
- This approximation makes
(Eq. 21) = 1; hence its use in Van der Ziel's (reference 3) “case (a)” does not seem justified.
