2021
DOI: 10.3390/ma14216639
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Burger Model as the Best Option for Modeling of Viscoelastic Behavior of Resists for Nanoimprint Lithography

Abstract: In this study, Atomic Force Microscopy-based nanoindentation (AFM-NI) with diamond-like carbon (DLC) coated tip was used to analyze the mechanical response of poly(methyl methacrylate) (PMMA) thin films (thicknesses: 235 and 513 nm) on a silicon substrate. Then, Oliver and Pharr (OP) model was used to calculate hardness and Young’s modulus, while three different Static Linear Solid models were used to fit the creep curve and measure creep compliance, Young’s modulus, and viscosity. Values were compared with ea… Show more

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Cited by 5 publications
(5 citation statements)
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“…In fact, viscosity experiments on thin films (80 – 500 nm) of PMMA ( T g ≈ 82°C) indicate a gradient layer structure in which the viscosity decreases from the glass/polymer to the polymer/air interface with an immobile layer adjacent to the glass and an intermediate glassy bulk layer and a mobile top layer, , a picture that fits our observations. T g increases by few °C when approaching the glass interface below a 100 nm distance; bulk viscosity is in the range of 10 9 Pa s, and viscous flow viscosities, i.e., of films at temperatures exceeding the polymer’s bulk T g , are in the 10 2 – 10 5 Pa s range . Our experiments demonstrate that SRG formation stops at the mobile layer and bulk layer interface, wherein the photonic force is unable to overcome the viscous force due to the large viscosity of the bulk layer.…”
Section: Resultsmentioning
confidence: 75%
See 1 more Smart Citation
“…In fact, viscosity experiments on thin films (80 – 500 nm) of PMMA ( T g ≈ 82°C) indicate a gradient layer structure in which the viscosity decreases from the glass/polymer to the polymer/air interface with an immobile layer adjacent to the glass and an intermediate glassy bulk layer and a mobile top layer, , a picture that fits our observations. T g increases by few °C when approaching the glass interface below a 100 nm distance; bulk viscosity is in the range of 10 9 Pa s, and viscous flow viscosities, i.e., of films at temperatures exceeding the polymer’s bulk T g , are in the 10 2 – 10 5 Pa s range . Our experiments demonstrate that SRG formation stops at the mobile layer and bulk layer interface, wherein the photonic force is unable to overcome the viscous force due to the large viscosity of the bulk layer.…”
Section: Resultsmentioning
confidence: 75%
“…T g increases by few °C when approaching the glass interface below a 100 nm distance; bulk viscosity is in the range of 10 9 Pa s, and viscous flow viscosities, i.e., of films at temperatures exceeding the polymer's bulk T g , are in the 10 2 − 10 5 Pa s range. 58 Our experiments demonstrate that SRG formation stops at the mobile layer and bulk layer interface, wherein the photonic force is unable to overcome the viscous force due to the large viscosity of the bulk layer. We will go on to discuss such competition between forces.…”
Section: Film Thicknessmentioning
confidence: 79%
“…Similarly, for the vacuum evaporation process, the inputs encompass the evaporation amount and resistance evaporation current, yielding the film thickness as the output. The predicted film thicknesses from both approaches are aggregated to obtain the overall predicted film thickness of the composite film [32,33].…”
Section: Feature Selection and Data Segmentationmentioning
confidence: 99%
“…In the field of biomedicine, SMNIL technology is widely used to construct micro and nanoscale biochips and laboratory on-a-chips, which play important roles in disease diagnosis, drug screening, biological analysis, and other fields [21][22][23].…”
Section: Biomedical Fieldmentioning
confidence: 99%