1957
DOI: 10.6028/jres.059.007
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Properties of arsenic sulfide glass

Abstract: Samples of ar~e n i c s ulfid e glaHS " -ere investigated to clc>lerll1ine the ir che m ical a nd phys ical properties. Amon g the proper ties r eported a re t ile hygros co pici t.I', chemi cal durability, hydroge n e lec trod e fUllc t ioll, ex pansivi ty , clastic nlOduli, modulus of rnpture', hardn ess, transmittance, and indices of re fraction .The main in te rest in "rse n ic s ulfid e glass, for t he prese n t, is for i ts lrnnslIliitance in t he i nfrared. It is transparent, t o infrared energy out to … Show more

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Cited by 43 publications
(8 citation statements)
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“…Assuming a point force deflection at the center of the cavity, we obtain the following equation for the force–distance relation of the rectangular membrane (see SI 4):where α( a , b ), C 2 ( a , b ), and c 0 ( a , b ) are geometry-dependent factors and N 0 is the intrinsic pretension. Using Poisson’s ratio ν 2 = 0.094, 49,50 we fit eq 1 to the data and extract effective Young’s moduli along the set of angles to the crystalline axes. We take into account measured thickness variations as determined by AFM, which are found to be at most one to two single layers (as seen in Figure 3a), to extract correct values of E eff .…”
Section: Resultsmentioning
confidence: 99%
“…Assuming a point force deflection at the center of the cavity, we obtain the following equation for the force–distance relation of the rectangular membrane (see SI 4):where α( a , b ), C 2 ( a , b ), and c 0 ( a , b ) are geometry-dependent factors and N 0 is the intrinsic pretension. Using Poisson’s ratio ν 2 = 0.094, 49,50 we fit eq 1 to the data and extract effective Young’s moduli along the set of angles to the crystalline axes. We take into account measured thickness variations as determined by AFM, which are found to be at most one to two single layers (as seen in Figure 3a), to extract correct values of E eff .…”
Section: Resultsmentioning
confidence: 99%
“…As 2 S 3 . Viscosity and the shear modulus data were published by Nemilov [49] and Glaze et al [65], respectively. The structural data on the crystalline form were taken from Vaipolin's review [66]: the mean distance d As-S = 2.23 ± 0.08 Å , the mean angle \S-As-S = a = 104.6 ± 3°.…”
Section: Appendix IImentioning
confidence: 99%
“…Also, the non-diagonal elements c 12 , c 13 , c 23 = λ together with their mirrored components. For thermal oxide, µ = 29.9 GPa, λ =15.4 GPa and ρ = 2.2 g/cm 3 [37], while As 2 S 3 is expectedly softer with µ = 6.2 GPa, λ = 9.78 GPa and ρ = 3.2 g/cm 3 [24], [38].…”
Section: Isotropic Materials:chalcogenidesmentioning
confidence: 99%