1954
DOI: 10.1021/ja01649a084
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Determination of Molecular Weights of Vapors at High Temperatures. I. The Vapor Pressure of Tin and the Molecular Weight of Tin Vapor1

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Cited by 47 publications
(18 citation statements)
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“…Ge and Sn were usually deposited with Knudsen cells in an ultrahigh vacuum (UHV) chamber. The calculated equilibrium vapor pressure of Sn is high, at 1.3 × 10 −10 and 6 × 10 −5 Pa at 500 and 800°C, respectively [27], while the melting point of Sn is very low, at 231.9°C. Hence, a crucible temperature as high as 800°C is often required to obtain a sufficiently high deposition rate.…”
Section: Molecular Beam Epitaxy (Mbe) Growth Of Ge 1−x Sn X Epitaxialmentioning
confidence: 87%
“…Ge and Sn were usually deposited with Knudsen cells in an ultrahigh vacuum (UHV) chamber. The calculated equilibrium vapor pressure of Sn is high, at 1.3 × 10 −10 and 6 × 10 −5 Pa at 500 and 800°C, respectively [27], while the melting point of Sn is very low, at 231.9°C. Hence, a crucible temperature as high as 800°C is often required to obtain a sufficiently high deposition rate.…”
Section: Molecular Beam Epitaxy (Mbe) Growth Of Ge 1−x Sn X Epitaxialmentioning
confidence: 87%
“…A liquid tin anode was specifically used due to its lower vapor pressure when compared to that of silver. [18,19] A molybdenum tube current collector was submerged in the liquid tin, and hydrogen gas was bubbled through the molybdenum tube at 30 cm 3 /min.…”
mentioning
confidence: 99%
“…1^/ and Volmer! !^' has subsequently been used by a large number of workg],g^ ( 15,16,(20)(21)(22)(23)(24)(25)(26)(27)(28)(29)(30)(31)(32)(33)(34) -jjj^g efforts of several of these workers are noteworthy with regard to the present work. Wessel!26) determined the vapor pressure of iron by employing effusion cells of quartz and alunaina suspended from a tungsten torsion wire in a graphite sheath furnace capable of operating at temperatures up to 1500°C.…”
Section: Experimental Techniquesmentioning
confidence: 92%
“…Upon substituting Equation (26), Equation (21) becomes dF^ = RTd In(aAp^) (27) or dF_4 = RTd lna_A + RTd Inp^ .…”
Section: Thermodynamicsmentioning
confidence: 99%