Recrystallization is a critical issue in ITER and future fusion devices as it strongly deteriorates the prop-erties and serving life of tungsten divertor *** this work,we investigated the influence of neon on the recr...
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Recrystallization is a critical issue in ITER and future fusion devices as it strongly deteriorates the prop-erties and serving life of tungsten divertor *** this work,we investigated the influence of neon on the recrystallization behavior of tungsten and its underlying mechanism by both experimental anal-ysis and molecular dynamics *** tungsten was irradiated by neon ion with energies of 10 and 100 keV and fluences of 1×10^(18)-1×10^(20)m^(−2),followed by isochronal annealing at various temperatures(1473-2073 K)for 1 *** results indicate that 10 keV neon ion irradiation slightly in-hibits tungsten recrystallization due to the shallow depth distribution of neon(35 nm),whereas 100 keV neon ion irradiation exerts a significant retarding effect on tungsten recrystallization when neon con-centration reaches∼102 *** boundaries can hardly move with neon concentration reaching 400 appm,above which the retarding effect is very strong and varies *** retarded recrystallization is mainly attributed to the pinning effect of neon clusters/bubbles on the grain boundary movement dur-ing *** neon clusters are found to play a predominant role in the retarding effect and the un-clustered neon atoms show a very limited effect on the grain boundary *** comparing the neon effects on recrystallization in this work and helium effects reported in the literature,we found that helium exhibits a relatively stronger recrystallization retarding effect than *** is because helium is more easily to diffuse into grain boundaries and form larger clusters due to its high diffusivity and low self-trapping energy in tungsten,which can greatly impede the migration of grain *** work provides a fundamental insight into the neon-concentration dependent recrystallization retarding effect in tungsten and the corresponding underlying atomic-level mechanisms.
Graph representation learning aims to represent graphs as vectors that can be utilized in downstream tasks such as graph classification. In this work, we focus on learning diverse representations that can capture the ...
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Graph representation learning aims to represent graphs as vectors that can be utilized in downstream tasks such as graph classification. In this work, we focus on learning diverse representations that can capture the graph information as much as possible. We propose quantifying graph information using graph entropy, where we define a probability distribution of a graph based on its nodes’ representations and global-graph representation. However, the computation of graph entropy is NP-hard due to the complex vertex-packing polytope involved in its definition. To address this challenge, we provide an approximation method leveraging orthonormal representations for graph entropy maximization. The proposed method is implemented via graph neural networks, resulting in informative node-level and graph-level representations. Experimental results demonstrate the effectiveness of our method in comparison to many baselines in unsupervised learning and semi-supervised learning tasks. The code of our method is available at https://***/MathAdventurer/GeMax. Copyright 2024 by the author(s)
This paper proposes a parallel framework for the Finite-Difference Time-Domain (FDTD) method on heterogeneous supercomputing platforms. The main content covers MPI parallelism, heterogeneous communication, and heterog...
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We study the structure of rings which satisfy the von Neumann regularity of commutators,and call a ring R C-regularif ab-ba ∈(ab-ba)R(ab-ba)for all a,b in *** a C-regular ring R,we prove J(R[X])=N^(*)(R[X])=N^(*)(R)[...
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We study the structure of rings which satisfy the von Neumann regularity of commutators,and call a ring R C-regularif ab-ba ∈(ab-ba)R(ab-ba)for all a,b in *** a C-regular ring R,we prove J(R[X])=N^(*)(R[X])=N^(*)(R)[X]=W(R)[X]■Z(R[X]),where J(A),N^(*)(A),W(A),Z(A)are the Jacobson radical,upper nilradical,Wedderburn radical,and center of a given ring A,respectively,and A[X]denotes the polynomial ring with a set X of commuting indeterminates over A;we also prove that R is semiprime if and only if the right(left)singular ideal of R is *** provide methods to construct C-regular rings which are neither commutative nor von Neumann regular,from any given ***,for a C-regular ring R,the following are proved to be equivalent:(i)R is Abelian;(ii)every prime factor ring of R is a duo domain;(ii)R is quasi-duo;and(iv)R/W(R)is reduced.
In this paper,we propose a simple energy decaying iterative thresholding algorithm to solve the two-phase minimum compliance *** material domain is implicitly represented by its characteristic function,and the problem...
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In this paper,we propose a simple energy decaying iterative thresholding algorithm to solve the two-phase minimum compliance *** material domain is implicitly represented by its characteristic function,and the problem is formulated into a minimization problem by the principle of minimum complementary *** prove that the energy is decreasing in each *** effective continuation schemes are proposed to avoid trapping into the local *** results on 2D isotropic linear material demonstrate the effectiveness of the proposed methods.
The coupling of excited states and ionic dynamics is the basic and challenging point for the materials response at extreme *** the laboratory,the intense laser produces transient nature and complexity with highly none...
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The coupling of excited states and ionic dynamics is the basic and challenging point for the materials response at extreme *** the laboratory,the intense laser produces transient nature and complexity with highly nonequilibrium states,making it extremely difficult and interesting for both experimental measurements and theoretical *** the inclusion of laser-excited states,we extend an ab initio method into the direct simulations of whole laser-driven microscopic dynamics from solid to *** construct the framework of combining the electron-temperature-dependent deep neural-network potential energy surface with a hybrid atomistic-continuum approach,controlling non-adiabatic energy exchange and atomistic dynamics,which enables consistent interpretation of experimental *** large-scale ab initio simulations,we demonstrate that the nonthermal effects introduced by hot electrons play a dominant role in modulating the lattice dynamics,thermodynamic pathway,and structural *** highlight that the present work provides a path to realistic computational studies of laser-driven processes,thus bridging the gap between experiments and simulations.
In this article, the interval type-3 fuzzy-based state feedback control is proposed for the stabilization problem of interval type-3 fuzzy systems (IT3FSs) subject to time-varying delay. Specifically, to improve the m...
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Frequency-comb emission via high-order harmonic generation(HHG)provides an alternative method for the coherent vacuum ultraviolet(VUV)and extreme ultraviolet(XUV)radiation at ultrahigh repetition *** particular,the te...
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Frequency-comb emission via high-order harmonic generation(HHG)provides an alternative method for the coherent vacuum ultraviolet(VUV)and extreme ultraviolet(XUV)radiation at ultrahigh repetition *** particular,the temporal and spectral features of the HHG were shown to carry profound insight into frequency-comb emission *** we present an ab initio investigation of the temporal and spectral coherence of the frequency comb emitted in HHG of He atom driven by few-cycle pulse *** find that the emission of frequency combs features a destructive and constructive coherences caused by the phase interference of HHG,leading to suppression and enhancement of frequency-comb *** results reveal intriguing and substantially different nonlinear optical response behaviors for frequency-comb emission via *** dynamical origin of frequency-comb emission is clarified by analyzing the phase coherence in HHG processes in *** results provide fresh insight into the experimental realization of selective enhancement of frequency comb in the VUV–XUV regimes.
We perform first-principles simulations to construct a multiphase equation of state (EOS) for magnesium (Mg) up to a pressure-temperature (P−T) range of 600 GPa and 8000 K. The phases considered include the solid hexa...
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We perform first-principles simulations to construct a multiphase equation of state (EOS) for magnesium (Mg) up to a pressure-temperature (P−T) range of 600 GPa and 8000 K. The phases considered include the solid hexagonal close-packed (hcp) and body-centered cubic (bcc) phases and the liquid phase. The effects of lattice anharmonicity on the free energies of the solid phases are considered using the phonon quasiparticle method, which is a hybrid approach that combines first-principles molecular dynamics (FPMD) and harmonic phonons to address lattice anharmonicity. These effects are found to significantly increase the calculated hcp-bcc transition pressure at high temperatures by >10% at T>1000 K and >20% at T>1250 K, leading to an hcp-bcc phase line in good overall agreement with static measurements. The free energies of the liquid phase are fitted using the results of FPMD simulations of this phase and constrained by our previous melting curve calculated from FPMD using the solid-liquid coexistence method. The resulting melting curve from our EOS reproduces the anomalous behavior of reentrant melting above ∼300 GPa from our previous calculations and shows better agreement with the results from shock experiments than with static measurements at high pressures. Our EOS places the hcp-bcc-liquid triple point at 25 GPa and 2030 K, higher in pressure and temperature than those from previous first-principles studies based on the quasiharmonic approximation (QHA). Comparisons are also made with other experimental data, including those from various static and shock experiments and generally indicate a high level of consistency.
A quantitative measure of symmetry breaking is introduced that allows the quantification of which symmetries are most strongly broken due to the introduction of some kind of defect in a perfect structure. The method u...
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