2015
DOI: 10.1063/1.4920925
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An exact formulation of the time-ordered exponential using path-sums

Abstract: We present the path-sum formulation for OE [H](t ′ , t) = T exp t ′ t H(τ ) dτ , the time-ordered exponential of a time-dependent matrix H(t). The path-sum formulation gives OE[H] as a branched continued fraction of finite depth and breadth. The terms of the path-sum have an elementary interpretation as selfavoiding walks and self-avoiding polygons on a graph. Our result is based on a representation of the time-ordered exponential as the inverse of an operator, the mapping of this inverse to sums of walks on g… Show more

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Cited by 43 publications
(57 citation statements)
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“…We would like a more nonperturbative approach, and we might hope that one exists since we are only dealing with finite-dimensional matrices rather than the infinite-dimensional Hilbert spaces familiar from other quantum systems like the harmonic oscillator. Indeed, such a nonperturbative method for finite-dimensional matrix equations was found in [49]. We employ their construction here.…”
Section: Analytics For N =mentioning
confidence: 99%
“…We would like a more nonperturbative approach, and we might hope that one exists since we are only dealing with finite-dimensional matrices rather than the infinite-dimensional Hilbert spaces familiar from other quantum systems like the harmonic oscillator. Indeed, such a nonperturbative method for finite-dimensional matrix equations was found in [49]. We employ their construction here.…”
Section: Analytics For N =mentioning
confidence: 99%
“…The operator T can be thought of as enforcing time order in the products for the standard exponential expansion in a sense which is equivalent to the power series definition, cf. [26]. Considering T e t 0 ∆ g(τ ) dτ as a formal power series, it is easy to see that the heat equation is satisfied.…”
Section: The Heat Kernel For (M G(·))mentioning
confidence: 99%
“…The graph underlying D is the periodic N × N mesh, so that we are in the presence of the general case this time, where the graph distance enters into the decay bounds. For N = 32, Figure 8 shows the exact decay for the 504th column of the inverse corresponding to the point (16, 24) on the mesh and the bounds given by Equation 17. The left part arranges the values according to a one-dimensional, lexicographic ordering of the mesh points, whereas the right part gives the same information arranged on the underlying two-dimensional mesh.…”
Section: Numerical Experimentsmentioning
confidence: 99%
“…14 There is much interest in finding bounds or estimates for the off-diagonal entries of matrix functions because these allow us to efficiently find sparse approximations of quantities of interest in a variety of areas such as Markov chain queuing models 15,16 and quantum dynamics. 17 Under certain conditions, for example, when the decay behavior is independent of the matrix size n for a family of matrices A n ∈ C n×n , the knowledge of sharp decay bounds even allows the design of optimal, linearly scaling algorithms for matrix function computations. 13,18 Thus, improving and extending results on off-diagonal decay in matrix functions are of great practical interest.…”
Section: Introductionmentioning
confidence: 99%