2022
DOI: 10.1016/j.cam.2021.113881
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An alternating-direction hybrid implicit-explicit finite-difference time-domain method for the Schrödinger equation

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Cited by 7 publications
(9 citation statements)
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“…e first step is to discretize space and time by dissecting the xt plane into a grid, where the x and t coordinates are divided into m and n equal parts; here, we have Δx � h � l/m, directional increment k � Δt, where l is the thickness of the specialized protective clothing fabric material layer, while we let i denote the position x transverse axis and j denote the transverse axis position t, with each grid point in the grid corresponding to one of its temperature values. Figure 2 shows the node diagram of the discrete post-finite difference manifold [18]. us, the temperature of the outer side of the dummy skin can be easily known in relation to the different thickness layers and the temperature distribution.…”
Section: Finite Difference Methods For Solving the One-dimensionalmentioning
confidence: 99%
See 1 more Smart Citation
“…e first step is to discretize space and time by dissecting the xt plane into a grid, where the x and t coordinates are divided into m and n equal parts; here, we have Δx � h � l/m, directional increment k � Δt, where l is the thickness of the specialized protective clothing fabric material layer, while we let i denote the position x transverse axis and j denote the transverse axis position t, with each grid point in the grid corresponding to one of its temperature values. Figure 2 shows the node diagram of the discrete post-finite difference manifold [18]. us, the temperature of the outer side of the dummy skin can be easily known in relation to the different thickness layers and the temperature distribution.…”
Section: Finite Difference Methods For Solving the One-dimensionalmentioning
confidence: 99%
“…In equation (18), K is the Boltzmann constant, T is the current absolute temperature, and P(Δf) is the probability of accepting the new state solution. At this point, there exists a random number c ∈ [0, 1], if P(Δf) > c, the new state arrangement is accepted; if P(Δf) ≤ c, the original state arrangement is retained.…”
Section: Study On the Optimization Model Of The Thickness Of Protecti...mentioning
confidence: 99%
“…Consequently, the system can be solved using the tridiagonal matrix algorithm as explained in [17], such that the complexity remains of linear order O(n) [33]. In Appendix B, the update scheme ( 16) is given in a more accessible scalar notation.…”
Section: B Electromagnetic Potentialsmentioning
confidence: 99%
“…The FDTD method is also popular in computational QM and has been applied to the Schrödinger or Kohn-Sham equations with many variations [9]- [14]. Implicit schemes such as [15], [16] have been recently improved by also including local implicitization [17]. Many implementations exist that couple the EM and QM problems [18]- [21], where, depending on the problem at hand, an effective-mass Schrödinger equation [22]- [26] or the ab initio Kohn-Sham equation [27]- [30] is considered.…”
Section: Introductionmentioning
confidence: 99%
“…Considering the components of the PIC, an optical switch is an important element that can work analogous to the electronic transistor in the electronic integrated circuits. Therefore, utmost efforts are made to achieve the functions of optical switching element using the time domain [16] or frequency domain [17], with different topologies in the form of cross waveguide geometries [18], quantum dots [19], optoelectronic hybrid devices [20], ring resonators [21], combined configurations of thermodynamics and optical components [22] and utilization of transparent and active materials [23,24], with it desired working and implementation in the optical circuits. A 2D-FDTD design of an optical switch is investigated in [25], by means of the phenomenon of GMR with varying radius cavity implemented at the start of the PhC-mesh.…”
Section: Introductionmentioning
confidence: 99%