2015
DOI: 10.1134/s1063783415050273
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Effect of a constant magnetic field on dislocation anharmonicity in silicon

Abstract: The effect of constant magnetic fields on dislocation anharmonicity of p type silicon single crys tals with a conductivity of 6 Ω cm has been studied. It has been found that preliminary exposure of dislocation silicon (with a dislocation density of 10 4 -10 6 cm -2 ) to a constant magnetic field (B = 0.7 T, t = 30 min) at room temperature causes a change in the nonlinear fourth order elastic modulus β d . The observed changes are associated with the dynamics of magnetosensitive complexes of structural defects … Show more

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Cited by 8 publications
(6 citation statements)
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“…where s T -Soret coefficient [6]. In addition to poor adhesion of the film to the substrate, the thermoelectric properties are affected by the volume defects of the structure.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…where s T -Soret coefficient [6]. In addition to poor adhesion of the film to the substrate, the thermoelectric properties are affected by the volume defects of the structure.…”
Section: Resultsmentioning
confidence: 99%
“…Analyzing the contact pairs with regard to new composition and geometry, one needs to pay attention primarily to the plot λ (∆t 1 ) on a pilot U -shaped curve of reliability [6], which represents the dependence of λ bounce from the time of operation of metallization t.…”
Section: Methodsmentioning
confidence: 99%
“…3. Plasticity of crystals can be changed by MF action before their deformation (i.e., the residual changes initiated by MF remain) [9,10].…”
Section: Introductionmentioning
confidence: 99%
“…Сьогодні відносно невеликою є кількість досліджень магнітозалежних явищ у кристалах кремнію у порівнянні із іншими слабомагнітними матеріалами, крім того більшість статей присвячені впливу пластичних деформацій на кремній n-типу провідності [12]. Тому актуальними залишаються дослідження по вивченні слабких пружних деформацій та магнітного поля на властивості кристалів p-Si [13,14]. Після дії магнітного поля, положення та величина характерного максимуму на кривих R/R0 = f(σ) залежить від часу, що пройшов від попереднього циклу деформації (рис.…”
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