Abstract:The elongation process under swift heavy ion irradiation (74 MeV Kr ions) of gold NPs, with a diameter in the range 10-30 nm, and embedded in a silica matrix has been investigated by combining experiment and simulation techniques: three-dimensional thermal spike (3DTS), molecular dynamics (MD) and a phenomenological simulation code specially developed for this study. 3DTS simulations evidence the formation of a track in the host matrix and the melting of the NP after the passage of the impinging ion. MD simula… Show more
“…An attempt to bridge this limitation was carried out by a new theoretical study, proposed to follow the complete shaping process for a wider range of Au NP sizes using a phenomenological simulation code based on the expansion/recrystallization mechanism observed by MD simulations [39]. As a result, it was concluded that the NP cannot completely expand into the matrix during the ion shaping process and should be limited by the time the track formation and the expansion process, suggesting that the matrix strongly resists the expansion of the Au NP afterwards.…”
We present the shape transformation of a single layer of Au NPs when embedded in, and at the interface of amorphous SiNx and SiOx (a-SiNx and a-SiOx) thin films upon irradiation with 185 MeV Au ions to fluences ranging from 0.3 to 30 × 10 13 cm -2 . Transmission electron microscopy (TEM) and high angular annular dark field (HAADF) microscopy were used to study the ion shaping process. The former allows us to follow the overall change in geometry, size and structure, while the latter reveals information about the relative position with respect to the interface. For Au NPs embedded in a single material, a lower elongation rate for a-SiNx was found in comparison to a-SiOx. When at the interface of the two materials, TEM reveals a preferential elongation towards a-SiOx. The latter demonstrates the use of a-SiNx for confining the ion-shaping process within an intermediate a-SiOx layer. The simulation of the temperature evolution during a single ion impact was used to understand the difference in elongation rates between a-SiNx and a-SiOx, as well as the asymmetric behaviour when located at the interface using the three-dimensional inelastic thermal spike (i-TS) model with bulk thermo-physical properties. The calculations show good agreement with the experimental observations and reveal a correlation between the thermal profile and the resulting NP geometry.
“…An attempt to bridge this limitation was carried out by a new theoretical study, proposed to follow the complete shaping process for a wider range of Au NP sizes using a phenomenological simulation code based on the expansion/recrystallization mechanism observed by MD simulations [39]. As a result, it was concluded that the NP cannot completely expand into the matrix during the ion shaping process and should be limited by the time the track formation and the expansion process, suggesting that the matrix strongly resists the expansion of the Au NP afterwards.…”
We present the shape transformation of a single layer of Au NPs when embedded in, and at the interface of amorphous SiNx and SiOx (a-SiNx and a-SiOx) thin films upon irradiation with 185 MeV Au ions to fluences ranging from 0.3 to 30 × 10 13 cm -2 . Transmission electron microscopy (TEM) and high angular annular dark field (HAADF) microscopy were used to study the ion shaping process. The former allows us to follow the overall change in geometry, size and structure, while the latter reveals information about the relative position with respect to the interface. For Au NPs embedded in a single material, a lower elongation rate for a-SiNx was found in comparison to a-SiOx. When at the interface of the two materials, TEM reveals a preferential elongation towards a-SiOx. The latter demonstrates the use of a-SiNx for confining the ion-shaping process within an intermediate a-SiOx layer. The simulation of the temperature evolution during a single ion impact was used to understand the difference in elongation rates between a-SiNx and a-SiOx, as well as the asymmetric behaviour when located at the interface using the three-dimensional inelastic thermal spike (i-TS) model with bulk thermo-physical properties. The calculations show good agreement with the experimental observations and reveal a correlation between the thermal profile and the resulting NP geometry.
“…A small elongation increment occurs after each impact. In a scenario supported by MD simulations 8,28 , the molten and expanding material from the NPs pushes to the underdense, molten track on top and beneath the nanoparticle on impact. Silica remains solid elsewhere when the ion trajectory intersects the NP from the center region.…”
Section: /22mentioning
confidence: 99%
“…Atomistic simulations performed by several groups have shown that NPs change shape on impacts 8,27,28,34 . On the other hand, the mere reproduction of the effect in the simulation does not unambiguously identify the underlying mechanism, and the conclusions drawn from MD simulations appear contradictory.…”
Section: /22mentioning
confidence: 99%
“…27 attribute the elongation to the formation of a shock wave, extremely high temperatures of the NP (9000K), and associated interfacial pressures. On the other hand, other authors 8,28,34 contribute the driving force to be the volume expansion due to melting and heating that occurs in considerably lower temperatures (2000K). Using first-principles MD computations, authors in Ref.…”
The shape of metal nanoparticles embedded in dielectric matrices influences the optical properties of the composite material. Swift heavy ion irradiation can induce a controllable shape transformation in gold and other metals embedded in amorphous silicon dioxide, where the particles elongate along the direction of the ion beam. The details of this transformation are not fully understood, but it is presumably related to nanometer-scale phase transitions induced by individual ion impacts. The phenomenon has been reproduced using atomistic simulations, although the time scale limitations and the lack of accurate interatomic models within the metal-silica interface lead unavoidably to severe simplifications.We improve the realism in the simulations with an accurate model for surface adhesion between gold and silica and by simulating the processes in the matrix between impacts. The simulations with correct adhesion show that the nanoparticles can grow in aspect ratio in the molten state even after silicon dioxide solidifies. Moreover, we demonstrate the active role of the matrix: without explicitly modeling processes in the matrix between impacts, the elongation is limited and does not reach significant aspect ratios seen in experiments. These results significantly improve the theoretical understanding of processes developing in embedded nanoparticles under swift heavy ion irradiation. The knowledge brings forward the ion beam technology as a precise tool for shaping of embedded nanostructures for various optical applications.
“…[ 74 ] To date, there are two major mechanisms proposed for the elongation: a) synergy effects by ion hammering and NP melting, [ 75–82 ] and b) ion shaping by ion tracks. [ 83–88 ] Ion hammering was discovered by Klaumunzer in 1983 that the NP dimensions grow (shrink) perpendicular (parallel) to the ion beam direction, which has been well understood by effective‐flow temperature approach. [ 89 ] In 2003, D'Orleans et al observed the ion shaping that spherical NPs become prolate with major axis oriented parallel to the incident direction.…”
Section: Ion Beam Synthesis Of Nanoparticlesmentioning
The zero‐dimensional metallic nanoparticles (NPs) have attracted tremendous attention in various areas owing to the collective oscillation of electron gas that couples with electromagnetic field, known as localized surface plasmon resonance (LSPR). In practical applications, the tailoring of LSPR effect is of significant importance for promising photonic devices with designed nanocomposite systems and enhanced optical properties. Ion beam technology has been demonstrated to be an efficient method to fabricate NPs embedded in dielectrics for LSPR tailoring and material modification. By manipulating the parameters of ion beams, the shape, size, and structure of NPs can be well controlled, which enables the dielectrics to possess novel linear and nonlinear optical properties. In this review, the latest research progress on the ion beam synthesis of various NPs is systematically summarized. The tailoring of linear and nonlinear optical properties of dielectrics by NPs is discussed in detail. Selected applications are presented to indicate the development of the plasmonic NPs in dielectric systems for photonic applications.
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