Modifying hydrogen-bonded structures by physical vapor deposition: 4-methyl-3-heptanol

We prepared films of 4-methyl-3-heptanol by vapor depositing onto substrates held at temperatures between T dep = 0.6T g and T g, where T g is the glass transition temperature. Using deposition rates between 0.9 and 6.0 nm/s, we prepared films about 5 μm thick and measured the dielectric properties...

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Veröffentlicht in:The Journal of chemical physics 2017-11, Vol.147 (19), p.194504-194504
Hauptverfasser: Young-Gonzales, A. R., Guiseppi-Elie, A., Ediger, M. D., Richert, R.
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container_issue 19
container_start_page 194504
container_title The Journal of chemical physics
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creator Young-Gonzales, A. R.
Guiseppi-Elie, A.
Ediger, M. D.
Richert, R.
description We prepared films of 4-methyl-3-heptanol by vapor depositing onto substrates held at temperatures between T dep = 0.6T g and T g, where T g is the glass transition temperature. Using deposition rates between 0.9 and 6.0 nm/s, we prepared films about 5 μm thick and measured the dielectric properties via an interdigitated electrode cell onto which films were deposited. Samples prepared at T dep = T g display the dielectric behavior of the ordinary supercooled liquid. Films deposited at lower deposition temperatures show a high dielectric loss upon heating toward T g, which decreases by a factor of about 12 by annealing at T g = 162 K. This change is consistent with either a drop of the Kirkwood correlation factor, g k , by a factor of about 10, or an increase in the dielectric relaxation times, both being indicative of changes toward ring-like hydrogen-bonded structure characteristic of the ordinary liquid. We rationalize the high dielectric relaxation amplitude in the vapor deposited glass by suggesting that depositions at low temperature provide insufficient time for molecules to form ring-like supramolecular structures for which dipole moments cancel. Surprisingly, above T g of the ordinary liquid, these vapor deposited films fail to completely recover the dielectric properties of the liquid obtained by supercooling. Instead, the dielectric relaxation remains slower and its amplitude much higher than that of the equilibrium liquid state, indicative of a structure that differs from the equilibrium liquid up to at least T g + 40 K.
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subjects Amplitudes
Correlation coefficients
Dielectric loss
Dielectric properties
Dielectric relaxation
Dipole moments
Glass transition temperature
Hydrogen bonding
Physical vapor deposition
Physics
Substrates
Supercooling
Thick films
Vapor deposited films
title Modifying hydrogen-bonded structures by physical vapor deposition: 4-methyl-3-heptanol
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