1970
DOI: 10.1070/pu1970v013n03abeh004256
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The Problem of High-Temperature Superconductivity. Ii

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Cited by 128 publications
(26 citation statements)
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“…If we let X = r (inner radius) --~ r (mean radius of nerve fiber) and A = thickness of dielectric lipid bilayer, using 0.434 for the ratio of log10x over logex , we may substitute equation 35 in equation 34 and obtain z~-6~ l-r (36) where Z is axon impedance for IR transmission in ohms and the other symbols are as previously defined.…”
Section: Vc~n = Vo -(Rt/f) Log [ Xr/(cx -X) J (25) Where Vo Is a Nementioning
confidence: 99%
“…If we let X = r (inner radius) --~ r (mean radius of nerve fiber) and A = thickness of dielectric lipid bilayer, using 0.434 for the ratio of log10x over logex , we may substitute equation 35 in equation 34 and obtain z~-6~ l-r (36) where Z is axon impedance for IR transmission in ohms and the other symbols are as previously defined.…”
Section: Vc~n = Vo -(Rt/f) Log [ Xr/(cx -X) J (25) Where Vo Is a Nementioning
confidence: 99%
“…Earlier suggestions for room temperature superconductivity come from (i) Little [16] and Ginzburg [17], where phonons which mediates attractive interactions is replaced by a high energy exciton of the polarizable medium, (ii) bipolaron route and (iii) metallic hydrogen (obtainable at ultra-high pressures), with a very high Debye frequency. Unfortunately, these suggestions have not materialized so for.…”
Section: Introductionmentioning
confidence: 99%
“…Sci. USA 85 (1988) earlier by several authors (50)(51)(52) and is being seriously considered in addition to models incorporating electroninduced charge exchange in the bonding orbitals (53). The third category incorporates electron coupling to spin fluctuations (54) and results in radically different thermodynamic properties.…”
Section: Methodsmentioning
confidence: 99%