1973
DOI: 10.1088/0022-3735/6/7/012
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Low temperature Hall measurements in a cryostat with a built-in magnet

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Cited by 12 publications
(7 citation statements)
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“…A Hall field (for the entire temperature range) orthogonal to the current density is applied to generate a voltage across the sample (1 × 1 cm 2 ) and called Hall voltage (V H ). From the Hall voltage (assuming one carrier conduction theory), the carrier density (n), resistivity (ρ), and Hall mobility (μ H ) can be calculated from the equations given below 35,36…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…A Hall field (for the entire temperature range) orthogonal to the current density is applied to generate a voltage across the sample (1 × 1 cm 2 ) and called Hall voltage (V H ). From the Hall voltage (assuming one carrier conduction theory), the carrier density (n), resistivity (ρ), and Hall mobility (μ H ) can be calculated from the equations given below 35,36…”
Section: Resultsmentioning
confidence: 99%
“…The nature of mobility indicates a predominant scattering by ionized impurities. 35 The overall mobility (μ) of the sample is represented as follows 42 In eq 6, μ p , μ dis , and μ imp are the mobility governed by phonon scattering, dislocation scattering in a semiconductor, and impurity scattering, respectively. Figure 6b shows temperature-dependent resistivity ρ(T) for untreated and treated carbon papers in a temperature range of 10−300 K. In both the samples, the resistivity decreases with an increase in temperature due to the increase of conductivity with temperature.…”
Section: R V T Ibmentioning
confidence: 99%
“…The static magnetic field was produced inside a helium gas-flow-cryostat by means of a small built-in electromagnet originally designed for low-temperature Hall measurenients [4]. The static field B= I_ 0.8 T was superimposed by a very weak a.c. field B sin wt (5 < B=).…”
Section: Methodsmentioning
confidence: 99%
“…La distorsion est inférieure à 0,1 %.2.2 LE CHAMP MAGNÉTIQUE. -Le champ magnétique est produit par un électro-aimant placé à l'intérieur du cryostat car cette disposition permet de minimiser les pertes et d'obtenir des champs intenses à fréquence élevée[10].Cet électro-aimant est constitué d'une bobine à noyau de ferrite (du type 3 C 8) où est taillé un entrefer de 2 mm dans lequel sera placé l'échantillon à mesurer. Le type de ferrite utilisée est prévu pour fonctionner à des fréquences élevées (allant jusqu'à 50 kHz); le meilleur rendement est obtenu à des fréquences voisines de 6 kHz.…”
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