Abstract:Molecular dynamics (MD) simulations have been carried out to examine the effects of Ar+, Ar+/H, and Ar+/F bombardment of a model polystyrene (PS) surface. For bombardment with 100 eV Ar+ only, the simulations show the formation of a heavily cross-linked dehydrogenated damaged layer in the near-surface region after some initial fluence, consistent with plasma and beam system experimental results. The 1–2 nm thick amorphous carbon-rich modified layer has a much lower sputter yield compared to that of the virgin … Show more
“…While the dependence of surface roughness on ion energy is opposite for PS and PMMA etched in Ar/O 2 , the surface roughness features are similar in size and form [12] suggesting that the same roughening mechanism is involved. The role of cross-linking is further explored through the use of alternate etch gas mixtures that are expected to suppress cross-linking [19]. Surface roughness of Ar/H 2 and Ar/F 2 etched PS and PMMA samples with four substrate bias voltages: −30 V to −150 V (ion energy: 45 eV to 165 eV) are shown in Figure 7.…”
Section: Resultsmentioning
confidence: 99%
“…In the case of PS, surface cross-linking is prevalent, while in PMMA, chain scissioning and depolymerization dominate [13,14,16]. While chemical structures such as the aromatic ring in PS and the methyl ester group in PMMA are commonly believed to play important roles in etching behaviors such as etch rate, cross-linking and chain scission, most studies reporting a correlation between chemical structures and etch behaviors of polymers are based on indirect observations, including change in molecular weight [16], etch rate [13,19], interface adhesion [14,16] or diffusion coefficient [20]. Details of the mechanisms involved have yet to be elucidated.…”
mentioning
confidence: 99%
“…In addition, while O 2 plasmas are found to enhance cross-linking during PS etching through formation of C-O-C bonds, H and F atoms were shown to suppress cross-linking during plasma etching [19]. H and F atoms form a single bond with C atoms, terminating dangling bonds and preventing cross-linking between C atoms in neighboring chains.…”
mentioning
confidence: 99%
“…Another set of experiments with Ar/H 2 and Ar/F 2 etching of PS and PMMA are designed to suppress the effects of cross-linking through the termination of dangling bonds by F or H atoms [19]. Post-etch roughness of PS samples with different MWs are also compared to investigate the contribution of intrinsic aggregation in surface roughening.…”
Selectively plasma-etched polystyrene-block-poly(methyl methacrylate) (PS-b-PMMA) diblock copolymer masks present a promising alternative for subsequent nanoscale patterning of underlying films. Because mask roughness can be detrimental to pattern transfer, this study examines roughness formation, with a focus on the role of cross-linking, during plasma etching of PS and PMMA. Variables include ion bombardment energy, polymer molecular weight and etch gas mixture. Roughness data support a proposed model in which surface roughness is attributed to polymer aggregation associated with cross-linking induced by energetic ion bombardment. In this model, RMS roughness peaks when cross-linking rates are comparable to chain scissioning rates, and drop to negligible levels for either very low or very high rates of cross-linking. Aggregation is minimal for very low rates of cross-linking, while very high rates produce a continuous cross-linked surface layer with low roughness. Molecular weight shows a negligible effect on roughness, while the introduction of H and F atoms suppresses roughness, apparently by terminating dangling bonds. For PS etched in Ar/O 2 plasmas, roughness decreases with increasing ion energy are tentatively attributed to the formation
OPEN ACCESSPolymers 2010, 2 650 of a continuous cross-linked layer, while roughness increases with ion energy for PMMA are attributed to increases in cross-linking from negligible to moderate levels.
“…While the dependence of surface roughness on ion energy is opposite for PS and PMMA etched in Ar/O 2 , the surface roughness features are similar in size and form [12] suggesting that the same roughening mechanism is involved. The role of cross-linking is further explored through the use of alternate etch gas mixtures that are expected to suppress cross-linking [19]. Surface roughness of Ar/H 2 and Ar/F 2 etched PS and PMMA samples with four substrate bias voltages: −30 V to −150 V (ion energy: 45 eV to 165 eV) are shown in Figure 7.…”
Section: Resultsmentioning
confidence: 99%
“…In the case of PS, surface cross-linking is prevalent, while in PMMA, chain scissioning and depolymerization dominate [13,14,16]. While chemical structures such as the aromatic ring in PS and the methyl ester group in PMMA are commonly believed to play important roles in etching behaviors such as etch rate, cross-linking and chain scission, most studies reporting a correlation between chemical structures and etch behaviors of polymers are based on indirect observations, including change in molecular weight [16], etch rate [13,19], interface adhesion [14,16] or diffusion coefficient [20]. Details of the mechanisms involved have yet to be elucidated.…”
mentioning
confidence: 99%
“…In addition, while O 2 plasmas are found to enhance cross-linking during PS etching through formation of C-O-C bonds, H and F atoms were shown to suppress cross-linking during plasma etching [19]. H and F atoms form a single bond with C atoms, terminating dangling bonds and preventing cross-linking between C atoms in neighboring chains.…”
mentioning
confidence: 99%
“…Another set of experiments with Ar/H 2 and Ar/F 2 etching of PS and PMMA are designed to suppress the effects of cross-linking through the termination of dangling bonds by F or H atoms [19]. Post-etch roughness of PS samples with different MWs are also compared to investigate the contribution of intrinsic aggregation in surface roughening.…”
Selectively plasma-etched polystyrene-block-poly(methyl methacrylate) (PS-b-PMMA) diblock copolymer masks present a promising alternative for subsequent nanoscale patterning of underlying films. Because mask roughness can be detrimental to pattern transfer, this study examines roughness formation, with a focus on the role of cross-linking, during plasma etching of PS and PMMA. Variables include ion bombardment energy, polymer molecular weight and etch gas mixture. Roughness data support a proposed model in which surface roughness is attributed to polymer aggregation associated with cross-linking induced by energetic ion bombardment. In this model, RMS roughness peaks when cross-linking rates are comparable to chain scissioning rates, and drop to negligible levels for either very low or very high rates of cross-linking. Aggregation is minimal for very low rates of cross-linking, while very high rates produce a continuous cross-linked surface layer with low roughness. Molecular weight shows a negligible effect on roughness, while the introduction of H and F atoms suppresses roughness, apparently by terminating dangling bonds. For PS etched in Ar/O 2 plasmas, roughness decreases with increasing ion energy are tentatively attributed to the formation
OPEN ACCESSPolymers 2010, 2 650 of a continuous cross-linked layer, while roughness increases with ion energy for PMMA are attributed to increases in cross-linking from negligible to moderate levels.
“…poly͑methyl methacrylate͒ ͑PMMA͒, 8 193 and 248 nm photoresists 5,6,9,10 ͔ and has been described as a thin, highly crosslinked and graphitized layer. [4][5][6][11][12][13][14][15][16] We have previously shown that under energetic Ar + ion bombardment during plasma etching, a dense, amorphous carbonlike modified layer is formed at the surface of a wide range of polymers ͓polystyrene ͑PS͒, poly͑␣-methylstyrene͒, poly͑4-methylstyrene͒, PMMA, poly͑hydroxyadamantyl acrylate͒, and poly͑hydroxyadaman-tyl methacrylate͔͒ with a thickness of a few nanometers. 17 This modified layer forms within the first few seconds of plasma exposure ͑corresponding to an ion fluence ϳ4 ϫ 10 16 cm −2 ͒, concurrent with a period of rapid surface roughening.…”
The uncontrolled development of nanoscale roughness during plasma exposure of polymer surfaces is a major issue in the field of semiconductor processing. In this paper, we investigated the question of a possible relationship between the formation of nanoscale roughening and the simultaneous introduction of a nanometer-thick, densified surface layer that is formed on polymers due to plasma damage. Polystyrene films were exposed to an Ar discharge in an inductively coupled plasma reactor with controllable substrate bias and the properties of the modified surface layer were changed by varying the maximum Ar + ion energy. The modified layer thickness, chemical, and mechanical properties were obtained using real-time in situ ellipsometry, x-ray photoelectron spectroscopy, and modeled using molecular dynamics simulation. The surface roughness after plasma exposure was measured using atomic force microscopy, yielding the equilibrium dominant wavelength and amplitude A of surface roughness. The comparison of measured surface roughness wavelength and amplitude data with values of and A predicted from elastic buckling theory utilizing the measured properties of the densified surface layer showed excellent agreement both above and below the glass transition temperature of polystyrene. This agreement strongly supports a buckling mechanism of surface roughness formation.
Organic one-dimensional nanostructures are attractive building blocks for electronic, optoelectronic, and photonic applications. Achieving aligned organic nanowire arrays that can be patterned on a surface with well-controlled spatial arrangement is highly desirable in the fabrication of high-performance organic devices. We demonstrate a facile one-step method for large-scale controllable patterning growth of ordered single-crystal C(60) nanowires through evaporation-induced self-assembly. The patterning geometry of the nanowire arrays can be tuned by the shape of the covering hats of the confined curve-on-flat geometry. The formation of the pattern arrays is driven by a simple solvent evaporation process, which is controlled by the surface tension of the substrate (glass or Si) and geometry of the evaporation surface. By sandwiching a solvent pool between the substrate and a covering hat, the evaporation surface is confined to along the edge of the solvent pool. The geometry of the formed nanowire pattern is well defined by a surface-tension model of the evaporation channel. This simple method is further established as a general approach that is applicable to two other organic nanostructure systems. The I-V characteristics of such a parallel, organic, nanowire-array device was measured. The results demonstrate that the proposed method for direct growth of nanomaterials on a substrate is a feasible approach to device fabrication, especially to the fabrication of the parallel arrays of devices.
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