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1.
Sheng Wu Gong Cheng Xue Bao ; 40(5): 1448-1468, 2024 May 25.
Artículo en Chino | MEDLINE | ID: mdl-38783808

RESUMEN

Nanoparticles, as a novel material, have a wide range of applications in the food and biomedical fields. Nanoparticles spontaneously adsorb proteins in the biological environment, and tens or even hundreds of proteins can form protein corona on the surface of nanoparticles. The formation of protein corona on the surface of nanoparticles is one of the key factors affecting the stability, biocompatibility, targeting, and drug release properties of nanoparticles. The formation mechanism of protein corona is affected by a variety of factors, including the surface chemical properties, sizes, and shapes of nanoparticles and the types, concentrations, and pH of proteins. Studies have shown that the protein structure is associated with protein distribution on the nanoparticle surface, while the protein conformation affects the binding mode and stability of the protein on the nanoparticle surface. Since the mechanism of the formation of protein corona on the surface of nanoparticles is complex, the roles of multiple factors need to be considered comprehensively. Understanding the mechanisms and influencing factors of the formation of protein corona will help us to understand the process of protein corona formation and control the formation of protein corona for specific needs. In this paper, we summarize the recent studies on the mechanisms and influencing factors of the formation of protein corona on the surface of nanoparticles, with a view to providing a theoretical basis for in-depth research on protein corona.


Asunto(s)
Nanopartículas , Corona de Proteínas , Propiedades de Superficie , Corona de Proteínas/química , Corona de Proteínas/metabolismo , Nanopartículas/química , Adsorción , Conformación Proteica , Humanos
2.
Adv Mater ; 36(18): e2310768, 2024 May.
Artículo en Inglés | MEDLINE | ID: mdl-38237911

RESUMEN

A charge density wave (CDW) represents an exotic state in which electrons are arranged in a long-range ordered pattern in low-dimensional materials. Although the understanding of the fundamental character of CDW is enriched after extensive studies, its practical application remains limited. Here, an unprecedented demonstration of a tunable charge-spin interconversion (CSI) in graphene/1T-TaS2 van der Waals heterostructures is shown by manipulating the distinct CDW phases in 1T-TaS2. Whereas CSI from spins polarized in all three directions is observed in the heterostructure when the CDW phase does not show commensurability, the output of one of the components disappears, and the other two are enhanced when the CDW phase becomes commensurate. The experimental observation is supported by first-principles calculations, which evidence that chiral CDW multidomains in the heterostructure are at the origin of the switching of CSI. The results uncover a new approach for on-demand CSI in low-dimensional systems, paving the way for advanced spin-orbitronic devices.

3.
Nano Lett ; 23(10): 4406-4414, 2023 May 24.
Artículo en Inglés | MEDLINE | ID: mdl-37140909

RESUMEN

Graphene is a light material for long-distance spin transport due to its low spin-orbit coupling, which at the same time is the main drawback for exhibiting a sizable spin Hall effect. Decoration by light atoms has been predicted to enhance the spin Hall angle in graphene while retaining a long spin diffusion length. Here, we combine a light metal oxide (oxidized Cu) with graphene to induce the spin Hall effect. Its efficiency, given by the product of the spin Hall angle and the spin diffusion length, can be tuned with the Fermi level position, exhibiting a maximum (1.8 ± 0.6 nm at 100 K) around the charge neutrality point. This all-light-element heterostructure shows a larger efficiency than conventional spin Hall materials. The gate-tunable spin Hall effect is observed up to room temperature. Our experimental demonstration provides an efficient spin-to-charge conversion system free from heavy metals and compatible with large-scale fabrication.

4.
Opt Lett ; 47(17): 4487-4490, 2022 Sep 01.
Artículo en Inglés | MEDLINE | ID: mdl-36048685

RESUMEN

A reconstruction design method for an aspherical recording system for varied line-space gratings is introduced. This method converts the recording system design from achieving specific groove distribution coefficients within the expansion model into reconstruction of the auxiliary mirror surface via the ray-tracing method. The effects of higher-order expansion terms in the expansion model are investigated and more accurate design of the varied line-space grating recording structure is achieved. By varying the surface reconstruction target, this method can be used to design aspherical recording structures with any auxiliary mirror surface shapes.

5.
Sci Adv ; 6(10): eaay2324, 2020 Mar.
Artículo en Inglés | MEDLINE | ID: mdl-32181344

RESUMEN

We have studied the charge to spin conversion in Bi1-x Sb x /CoFeB heterostructures. The spin Hall conductivity (SHC) of the sputter-deposited heterostructures exhibits a high plateau at Bi-rich compositions, corresponding to the topological insulator phase, followed by a decrease of SHC for Sb-richer alloys, in agreement with the calculated intrinsic spin Hall effect of Bi1-x Sb x . The SHC increases with increasing Bi1-x Sb x thickness before it saturates, indicating that it is the bulk of the alloy that predominantly contributes to the generation of spin current; the topological surface states, if present, play little role. Unexpectedly, the SHC is found to increase with increasing temperature, following the trend of carrier density. These results suggest that the large SHC at room temperature, with a spin Hall efficiency exceeding 1 and an extremely large spin current mobility, is due to increased number of thermally excited Dirac-like electrons in the L valley of the narrow gap Bi1-x Sb x alloy.

6.
Phys Rev Lett ; 113(11): 119601, 2014 Sep 12.
Artículo en Inglés | MEDLINE | ID: mdl-25260010

RESUMEN

A Comment on the Letter by B. Xu and X. Chen, Phys. Rev. Lett. 110, 156103 (2013).

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