2017
DOI: 10.1007/978-3-319-64191-1
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Tensor Network States and Effective Particles for Low-Dimensional Quantum Spin Systems

Abstract: Zo hoort de theoretische fysica te zijn, geen verpleeghuis voor kreupelen, maar een speelplaats voor gezonde, vitale, bloeiende, lachende, vrolijke losbollen, welgeschapen, complete wezens die tevreden zijn met zichzelf, die ieder voor zich het ideaalbeeld zijn van hun moeder en de kracht van hun vaders lendenen, niet de misgeboorten van vage wensen, niet de nageboorte die met de naweeën komt. Het onderhavige werk is het resultaat van vier jaar vertoeven op deze speelplaats die theoretische fysica heet, en ik … Show more

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Cited by 11 publications
(13 citation statements)
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“…The blocks decrease exponentially as we go further from the diagonal, so we can, in order to solve the problem, consider them to be zero if |n − n | > M for a sufficiently large M . In this approximation, the coefficients c(n) obey From the special structure of the blocks A m [49] and their relation to the effective one-particle hamiltonian H eff (p), we already know a number of solutions to Eq. (219).…”
Section: Asymptotic Regimementioning
confidence: 99%
See 1 more Smart Citation
“…The blocks decrease exponentially as we go further from the diagonal, so we can, in order to solve the problem, consider them to be zero if |n − n | > M for a sufficiently large M . In this approximation, the coefficients c(n) obey From the special structure of the blocks A m [49] and their relation to the effective one-particle hamiltonian H eff (p), we already know a number of solutions to Eq. (219).…”
Section: Asymptotic Regimementioning
confidence: 99%
“…the relative group velocity in the center of mass frame. Much like the proof of conservation of particle current in one-particle quantum mechanics, it can be shown [49] that, if (230) is to be the asymptotic form of an eigenstate, the coefficients r γ i (P, ω) should obey γ r γ i (P, ω) 2 dω γ dp (p γ ) = 0.…”
Section: S Matrix and Normalizationmentioning
confidence: 99%
“…Recently AD techniques have been applied to the optimization problem of iPEPS [10]. Considerable effort has been put into development of powerful yet efficient optimization algorithms for iPEPS in recent years, from very inexpensive [35] though generally less accurate or more balanced [1,3,31] imaginary time evolution methods to powerful though more expensive variational optimization approaches [36,37]. While these methods form a broad and widely applicable set of tools, AD offers a compelling alternative since it essentially does not require the implementation of any optimization algorithm at all, but only a routine for contracting the network and computing expectation values.…”
Section: Automatic Differentiationmentioning
confidence: 99%
“…In all cases, the correlations between such DoF underpin the low-energy properties of the model. We note that similar ideas have recently been used in the framework of matrix product state methods in order to construct quasiparticle excitations in various 1D models [39][40][41] .…”
Section: Fig 1 (A)mentioning
confidence: 99%