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A Space-Time Continuous Galerkin Finite Element Method for Linear Schrödinger Equations

Marco Zank

TL;DR

The paper presents an $H^1$-conforming space-time Galerkin finite element method for the linear Schrödinger equation $i \partial_t \psi - \Delta_x \psi = f$ with Dirichlet data, using a tensor-product discretization in time and space. The global system $$(i B_t \otimes M_x + M_t \otimes A_x) \boldsymbol{\psi} = \boldsymbol{f}$$ is solved via Kronecker-structured direct solvers, either Bartels–Stewart (Schur decomposition) or the fast diagonalization method, enabling parallelization across time through independent spatial solves. Numerical experiments on a 2D unit square demonstrate second-order convergence in $L^2(Q)$ and first-order convergence in $H^1(Q)$, with significant speedups when employing the fast diagonalization approach, even on nonuniform temporal meshes. The findings indicate that time-parallel direct solvers for space-time FEMs offer a practical route to efficient quantum-dynamics simulations on Lipschitz domains.

Abstract

We introduce a space-time finite element method for the linear time-dependent Schrödinger equation with Dirichlet conditions in a bounded Lipschitz domain. The proposed discretization scheme is based on a space-time variational formulation of the time-dependent Schrödinger equation. In particular, the space-time method is conforming and is of Galerkin-type, i.e., trial and test spaces are equal. We consider a tensor-product approach with respect to time and space, using piecewise polynomial, continuous trial and test functions. In this case, we state the global linear system and efficient direct space-time solvers based on exploiting the Kronecker structure of the global system matrix. This leads to the Bartels-Stewart method and the fast diagonalization method. Both methods result in solving a sequence of spatial subproblems. In particular, the fast diagonalization method allows for solving the spatial subproblems in parallel, i.e., a time parallelization is possible. Numerical examples for a two-dimensional spatial domain illustrate convergence in space-time norms and show the potential of the proposed solvers.

A Space-Time Continuous Galerkin Finite Element Method for Linear Schrödinger Equations

TL;DR

The paper presents an -conforming space-time Galerkin finite element method for the linear Schrödinger equation with Dirichlet data, using a tensor-product discretization in time and space. The global system is solved via Kronecker-structured direct solvers, either Bartels–Stewart (Schur decomposition) or the fast diagonalization method, enabling parallelization across time through independent spatial solves. Numerical experiments on a 2D unit square demonstrate second-order convergence in and first-order convergence in , with significant speedups when employing the fast diagonalization approach, even on nonuniform temporal meshes. The findings indicate that time-parallel direct solvers for space-time FEMs offer a practical route to efficient quantum-dynamics simulations on Lipschitz domains.

Abstract

We introduce a space-time finite element method for the linear time-dependent Schrödinger equation with Dirichlet conditions in a bounded Lipschitz domain. The proposed discretization scheme is based on a space-time variational formulation of the time-dependent Schrödinger equation. In particular, the space-time method is conforming and is of Galerkin-type, i.e., trial and test spaces are equal. We consider a tensor-product approach with respect to time and space, using piecewise polynomial, continuous trial and test functions. In this case, we state the global linear system and efficient direct space-time solvers based on exploiting the Kronecker structure of the global system matrix. This leads to the Bartels-Stewart method and the fast diagonalization method. Both methods result in solving a sequence of spatial subproblems. In particular, the fast diagonalization method allows for solving the spatial subproblems in parallel, i.e., a time parallelization is possible. Numerical examples for a two-dimensional spatial domain illustrate convergence in space-time norms and show the potential of the proposed solvers.

Paper Structure

This paper contains 5 sections, 1 theorem, 26 equations, 1 figure, 3 tables.

Key Result

Theorem 1

Let the given right-hand side $f \in L^2(Q)$ satisfy the condition and let the given initial data $\psi_0 \in H^1_0(\Omega)$. Then, a unique solution $\psi \in W(Q)$ to the time-de-pen-dent Schrö-ding-er equation (zank:SchroedingerBeschraenkt) exists such that the regularity results hold true.

Figures (1)

  • Figure 1: Initial spatial mesh for $\Omega = (0,1) \times (0,1)$ and initial temporal meshes for $T=5$.

Theorems & Definitions (2)

  • Theorem 1
  • proof