2022
DOI: 10.1021/acs.jctc.2c00209
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Tensor-Train Split-Operator KSL (TT-SOKSL) Method for Quantum Dynamics Simulations

Abstract: Numerically exact simulations of quantum reaction dynamics, including nonadiabatic effects in excited electronic states, are essential to gain fundamental insights into ultrafast chemical reactivity and rigorous interpretations of molecular spectroscopy. Here, we introduce the tensor-train split-operator KSL (TT-SOKSL) method for quantum simulations in tensor-train (TT)/matrix product state (MPS) representations. TT-SOKSL propagates the quantum state as a tensor train using the Trotter expansion of the time-ev… Show more

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Cited by 26 publications
(25 citation statements)
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“…In the projector-splitting algorithm, the wavepacket propagation is achieved by the orthogonal projection onto the tangent space given by a predefined MPS manifold. More detailed discussions on this algorithm were found in previous works. , The error minimization can be achieved by the definition of the orthogonal projection of the evolution vector onto the tangent space given by a predefined MPS manifold where Ψ­( t ) denotes the total wave function, P̂ T ,|Ψ( t )⟩ is the orthogonal projector on the tangent space, which can be decomposed into two terms using the left projector P̂ i L and right projector P̂ i R In practice, the above equation of motion can be solved approximately by solving m forward-evolving equations and ( m – 1) backward-evolving equations individually and sequentially The reduced density matrix for the electronic part is given by the following equation where the diagonal ( i = j ) and off-diagonal ( i ≠ j ) elements represent the electronic populations and coherences, respectively.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…In the projector-splitting algorithm, the wavepacket propagation is achieved by the orthogonal projection onto the tangent space given by a predefined MPS manifold. More detailed discussions on this algorithm were found in previous works. , The error minimization can be achieved by the definition of the orthogonal projection of the evolution vector onto the tangent space given by a predefined MPS manifold where Ψ­( t ) denotes the total wave function, P̂ T ,|Ψ( t )⟩ is the orthogonal projector on the tangent space, which can be decomposed into two terms using the left projector P̂ i L and right projector P̂ i R In practice, the above equation of motion can be solved approximately by solving m forward-evolving equations and ( m – 1) backward-evolving equations individually and sequentially The reduced density matrix for the electronic part is given by the following equation where the diagonal ( i = j ) and off-diagonal ( i ≠ j ) elements represent the electronic populations and coherences, respectively.…”
Section: Methodsmentioning
confidence: 99%
“…More detailed discussions on this algorithm were found in previous works. 109,110 The error minimization can be achieved by the definition of the orthogonal projection of the evolution vector onto the tangent space given by a predefined MPS manifold…”
Section: Tensor-trainmentioning
confidence: 99%
“…However, numerically exact full-quantum methods such as numerically exact wavepacket propagation approaches , are usually only feasible to a small number of degrees of freedom (DoFs) due to the curse of dimensionality. Through decomposing the wave function of a large high-rank tensor into the product of many small low-rank tensors, the time-dependent density matrix renormalization group (TD-DMRG) and multiconfigurational time-dependent Hartree (MCTDH) as well as its multilayer variant (ML-MCTDH) , increased the computational efficiency remarkably and made it feasible to simulate the dynamics of excitonic systems with up to a few hundred vibrational or phonon DoFs. This promotes the full QD simulations of nonadiabatic processes in realistic molecules with up to a few tens of atoms, ranging from charge transfer or energy transfer to singlet fission …”
Section: Introductionmentioning
confidence: 99%
“…The developed technique has a resemblance with the methods based on the propagation of the matrix product states, tree tensor networks, and density matrix renormalization group formalism useful in different quantum chemical/dynamical applications. These methods are formulated for the wave function of a quantum state, instead we consider here the time-evolution of the surprisal. The proposed route is highly efficient for the propagation of the states of maximal entropy (subject to constraints), providing exceedingly small number of the time-dependent coefficients for the coherent multi-electronic state dynamics. …”
Section: Introductionmentioning
confidence: 99%