1985
DOI: 10.1002/pssa.2210910146
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Effect of High-Temperature Annealing on Phonon-Phonon Relaxation in Transmutationally-Doped Silicon Crystals

Abstract: This short communication a i m s a t elucidating the effect of high-temperature (HT) annealing on the phonon-phonon relaxation in transmutationally-doped (TD) n-Si crystals. The relaxation is known to govern not only the value but also the anisotropy of the heat e. m. f. caused by the drag of electrons by phonons of longitudinal (1) and transverse (t) polarization.In our study we used TD c r y s t a l s of n-Si which, apart from the common technological annealing (T = 800 OC, t = 2 h), were exposed to HT annea… Show more

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“…It is known that at low concentrations of charge carriers ( n ≤ 10 15 cm −3 ), the phonon and diffusive (electronic) components of thermo‐emf are additive , and the thermo‐emf anisotropy in the region of impurity conduction (i.e., in condition of one kind of carriers, even if the anisotropy of their effective mass is strongly expressed) is entirely determined only by the anisotropy of the phonon component : αph=ααnormale, where α is the experimentally measured thermo‐emf; α e is the electronic (diffusive) component of thermo‐emf; α ph is the component of thermo‐emf associated with drag of electrons by phonons. Anisotropy of drag thermo‐emf in cubic crystals is determined by difference of the phonon components of thermo‐emf along and across of the main axis of isoenergetic ellipsoid, i.e., Δα=α||phαph, whereas the anisotropy parameter of drag thermo‐emf is determined by their ratio M=α||ph/αph. …”
Section: Temperature Dependence Of the Anisotropy Parameter Of Drag Tmentioning
confidence: 99%
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“…It is known that at low concentrations of charge carriers ( n ≤ 10 15 cm −3 ), the phonon and diffusive (electronic) components of thermo‐emf are additive , and the thermo‐emf anisotropy in the region of impurity conduction (i.e., in condition of one kind of carriers, even if the anisotropy of their effective mass is strongly expressed) is entirely determined only by the anisotropy of the phonon component : αph=ααnormale, where α is the experimentally measured thermo‐emf; α e is the electronic (diffusive) component of thermo‐emf; α ph is the component of thermo‐emf associated with drag of electrons by phonons. Anisotropy of drag thermo‐emf in cubic crystals is determined by difference of the phonon components of thermo‐emf along and across of the main axis of isoenergetic ellipsoid, i.e., Δα=α||phαph, whereas the anisotropy parameter of drag thermo‐emf is determined by their ratio M=α||ph/αph. …”
Section: Temperature Dependence Of the Anisotropy Parameter Of Drag Tmentioning
confidence: 99%
“…It was necessary to clarify the change character of thermo‐emf anisotropy Δ α and parameter M in n‐Si crystals with temperature, having taken into account the proof of a determinative role of the drag along the main axis of isoenergetic ellipsoid (α||true(l,ttrue)αtrue(l,ttrue)), obtained in Ref. , and the prevailing significance of the electron drag under the influence of the longitudinal polarization phonons (α||,true(ltrue)>α||,true(ttrue)) at the given direction with regard to the axes of ellipsoid.…”
Section: Temperature Dependence Of the Anisotropy Parameter Of Drag Tmentioning
confidence: 99%
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