2015
DOI: 10.1140/epjd/e2015-60129-1
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Collision of atoms with porous polymer surface: evidence of influence of bulk diffusion on anomalously long dwell time of Rb atoms

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Cited by 1 publication
(3 citation statements)
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“…According to the Stokes -Einstein equation, which describes diffusivity to be inverse proportional to viscosity, one can speculate that on the surface of a completely polymerized PDMS with viscosity enhanced one million times, the dwell time should be one million times smaller: 10 -4 /10 6 = 10 -10 s. This is true if the polymerization does not change the attractive potential barrier on the cured PDMS film surface. Note that this estimated dwell time value is close to the one derived from the measured potential barrier on the film surface and the film temperature [19].…”
Section: The Question Ariseswhat Has Happened With the Coating During...supporting
confidence: 80%
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“…According to the Stokes -Einstein equation, which describes diffusivity to be inverse proportional to viscosity, one can speculate that on the surface of a completely polymerized PDMS with viscosity enhanced one million times, the dwell time should be one million times smaller: 10 -4 /10 6 = 10 -10 s. This is true if the polymerization does not change the attractive potential barrier on the cured PDMS film surface. Note that this estimated dwell time value is close to the one derived from the measured potential barrier on the film surface and the film temperature [19].…”
Section: The Question Ariseswhat Has Happened With the Coating During...supporting
confidence: 80%
“…We estimate how deep atoms can diffuse inside a fresh polymer film l during a dwell time d. For instance, in the case of rubidium and PDMS, we have Dp =1.1•10 -3 cm 2 /sec (that is found by extrapolation the curve in Fig.2 to zero time), d =10 -4 sec from [19] and by using the…”
Section: Fig 3 Diffusion Coefficient Dp Versus Curing Timementioning
confidence: 87%
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