Bulletin of the American Physical Society
2024 APS March Meeting
Monday–Friday, March 4–8, 2024; Minneapolis & Virtual
Session A32: Molecular Glasses: Dynamics
8:00 AM–11:00 AM,
Monday, March 4, 2024
Room: 102D
Sponsoring
Unit:
DPOLY
Chair: Sarah Wolf, SUNY Cortland
Abstract: A32.00001 : Anatomy of a vapor deposited glass*
8:00 AM–8:36 AM
Presenter:
Ranko Richert
(Arizona State University)
Authors:
Ranko Richert
(Arizona State University)
Megan Tracy
(University of Wisconsin - Madison)
Mark D Ediger
(University of Wisconsin - Madison)
During and after deposition, the dielectric permittivity of MMT films has been measured with a resolution of tanδ = 10-7 via an interdigitated electrode structure with a geometric capacitance of 2.2 pF. In all cases, the capacitance of the cell rose linearly with time, indicative of a constant deposition rate. During deposition, the dielectric loss of the film rises quickly at first, and then near linearly with time. The analysis of these deposition curves reveals a slightly different structure near the substrate, a bulk of the film that does not change the loss behavior for 50,000 s after deposition, and a surface layer of more mobile material. The thickness of this layer is at or below 1 nm for deposition at low temperature and sharply rises to above 10 nm average thickness at Tg. The dielectric loss, ε'', understood as indicator of the fictive temperature Tfic, is observed to change gradually from the mobile surface with Tfic > Tg to the much lower value of the stable glass, where Tfic is assumed to be close to the deposition temperature. After the deposition had stopped, this mobile surface layer undergoes considerable reduction of its dielectric loss, and this annealing effect is believed to arise from material positioned 5 to 30 nm below the surface. The picture of a fictive temperature gradient near the surface as derived from these observations differs from that of a distinct mobile layer that quickly and directly converts to the kinetically stable glass.
*This work was supported by the National Science Foundation under Grant No. CHE- 2153944.
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