TY - JOUR
T1 - Over What Length Scale Does an Inorganic Substrate Perturb the Structure of a Glassy Organic Semiconductor?
AU - Bagchi, Kushal
AU - Deng, Chuting
AU - Bishop, Camille
AU - Li, Yuhui
AU - Jackson, Nicholas E.
AU - Jackson, Nicholas E.
AU - Yu, Lian
AU - Yu, Lian
AU - Toney, M. F.
AU - De Pablo, J. J.
AU - De Pablo, J. J.
AU - Ediger, M. D.
N1 - Funding Information:
The experimental portion of this work was supported by the US Department of Energy, Office of Basic Energy Sciences, Division of Materials Sciences and Engineering, Award DE-SC0002161. The authors gratefully acknowledge use of facilities and instrumentation supported by NSF through the University of Wisconsin Materials Research Science and Engineering Center (DMR-1720415). Use of the Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, is supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract DE-AC02-76SF00515. The molecular simulations presented in this work were performed at Argonne National Laboratory with support from the Department of Energy, Office of Science, Basic Energy Sciences, Division of Materials Science and Engineering.
Publisher Copyright:
Copyright © 2020 American Chemical Society.
PY - 2020/6/10
Y1 - 2020/6/10
N2 - While the bulk structure of vapor-deposited glasses has been extensively studied, structure at buried interfaces has received little attention, despite being important for organic electronic applications. To learn about glass structure at buried interfaces, we study the structure of vapor-deposited glasses of the organic semiconductor DSA-Ph (1,4-di-[4-(N,N-diphenyl)amino]styrylbenzene) as a function of film thickness; the structure is probed with grazing incidence X-ray scattering. We deposit on silicon and gold substrates and span a film thickness range of 10-600 nm. Our experiments demonstrate that interfacial molecular packing in vapor-deposited glasses of DSA-Ph is more disordered compared to the bulk. At a deposition temperature near room temperature, we estimate ∼8 nm near the substrate can have modified molecular packing. Molecular dynamics simulations of a coarse-grained representation of DSA-Ph reveal a similar length scale. In both the simulations and the experiments, deposition temperature controls glass structure beyond this interfacial layer of a few nanometers.
AB - While the bulk structure of vapor-deposited glasses has been extensively studied, structure at buried interfaces has received little attention, despite being important for organic electronic applications. To learn about glass structure at buried interfaces, we study the structure of vapor-deposited glasses of the organic semiconductor DSA-Ph (1,4-di-[4-(N,N-diphenyl)amino]styrylbenzene) as a function of film thickness; the structure is probed with grazing incidence X-ray scattering. We deposit on silicon and gold substrates and span a film thickness range of 10-600 nm. Our experiments demonstrate that interfacial molecular packing in vapor-deposited glasses of DSA-Ph is more disordered compared to the bulk. At a deposition temperature near room temperature, we estimate ∼8 nm near the substrate can have modified molecular packing. Molecular dynamics simulations of a coarse-grained representation of DSA-Ph reveal a similar length scale. In both the simulations and the experiments, deposition temperature controls glass structure beyond this interfacial layer of a few nanometers.
KW - GIWAXS
KW - buried interface
KW - coarse-grained simulations
KW - organic light-emitting diode
KW - organic semiconductor
KW - organic-inorganic interface
KW - ultrathin films
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U2 - 10.1021/acsami.0c06428
DO - 10.1021/acsami.0c06428
M3 - Article
C2 - 32402187
AN - SCOPUS:85086345859
SN - 1944-8244
VL - 12
SP - 26717
EP - 26726
JO - ACS Applied Materials and Interfaces
JF - ACS Applied Materials and Interfaces
IS - 23
ER -