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arXiv:1505.06083 · New Journal of Physics

Diverging scaling with converging multisite entanglement in odd and even quantum Heisenberg ladders

Sudipto Singha Roy, Himadri Shekhar Dhar, Debraj Rakshit, Aditi Sen, Ujjwal Sen

Published Feb 4, 2016• 9 citations
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Abstract

We investigate finite-size scaling of genuine multisite entanglement in the ground state of quantum spin-1/2 Heisenberg ladders. We obtain the ground states of odd- and even-legged Heisenberg ladder Hamiltonians and compute genuine multisite entanglement, the generalized geometric measure (GGM), which shows that for even rungs, GGM increases for odd-legged ladder while it decreases for even ones. Interestingly, the ground state obtained by short-range dimer coverings, under the resonating valence bond ansatz, encapsulates the qualitative features of GGM for both the ladders. We find that while the quantity converges to a single value for higher legged odd- and even-ladders, in the asymptotic limit of a large number of rungs, the finite-size scaling exponents of the same tend to diverge. The scaling exponent of GGM is therefore capable to distinguish the odd–even dichotomy in Heisenberg ladders, even when the corresponding multisite entanglements merge. Introduction and background . The sequences of odd and even numbers mathematically reach the same infinity. The question is whether limits of functions of odd/even numbers reach the same limiting function as the respective sequences tend to infinity. In many-body physics, the dichotomy between physical properties of odd and even quantum ladders is known, and a typical result is exemplified by the seminal work of White, Noack, and Scalapino (PRL 73,886 (1994)), wherein the spin gap was shown to exhibit different behaviors in odd and even ladders. The values of the spin gaps were shown as converging to a single value with the increase in the number of legs, irrespective of whether we are with odd or even ladders. It may now be asked whether one can identify a physical quantity that would have different limiting values depending on whether odd or even legged ladders are followed to reach the infinite 2D square lattice. We answer this query in the affirmative by identifying the scaling of multisite entanglement as the physical quantity that is capable of doing the job. Main results . We evaluate the asymptotic genuine multisite entanglement of states of quantum spin models on ladder lattices with odd and even legs, and perform finite size scaling analysis of the same. We find that scaling exponents of the multisite entanglement for large lattices tend to diverge for odd and even ladders, as the number of legs are increased, even though the amount of the multisite entanglement converges in the asymptotic limit. Wider implications . We believe that the results presented in the manuscript will be of interest to the broad physics community working on stronglycorrelated systems, quantum information in many-body physics, and related quantum technologies. The methodology presented in the manuscript will, we believe, also appeal to the general theoretical physics community.

DOI
10.1088/1367-2630/18/2/023025

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We investigate finite-size scaling of genuine multisite entanglement in the ground state of quantum spin-1/2 Heisenberg ladders. We obtain the ground states of odd- and even-legged Heisenberg ladder Hamiltonians and compute genuine multisite entanglement, the generalized geometric measure (GGM), which shows that for even rungs, GGM increases for odd-legged ladder while it decreases for even ones. Interestingly, the ground state obtained by short-range dimer coverings, under the resonating valence bond ansatz, encapsulates the qualitative features of GGM for both the ladders. We find that while the quantity converges to a single value for higher legged odd- and even-ladders, in the asymptotic limit of a large number of rungs, the finite-size scaling exponents of the same tend to diverge. The scaling exponent of GGM is therefore capable to distinguish the odd–even dichotomy in Heisenberg ladders, even when the corresponding multisite entanglements merge. Introduction and background . The sequences of odd and even numbers mathematically reach the same infinity. The question is whether limits of functions of odd/even numbers reach the same limiting function as the respective sequences tend to infinity. In many-body physics, the dichotomy between physical properties of odd and even quantum ladders is known, and a typical result is exemplified by the seminal work of White, Noack, and Scalapino (PRL 73,886 (1994)), wherein the spin gap was shown to exhibit different behaviors in odd and even ladders. The values of the spin gaps were shown as converging to a single value with the increase in the number of legs, irrespective of whether we are with odd or even ladders. It may now be asked whether one can identify a physical quantity that would have different limiting values depending on whether odd or even legged ladders are followed to reach the infinite 2D square lattice. We answer this query in the affirmative by identifying the scaling of multisite entanglement as the physical quantity that is capable of doing the job. Main results . We evaluate the asymptotic genuine multisite entanglement of states of quantum spin models on ladder lattices with odd and even legs, and perform finite size scaling analysis of the same. We find that scaling exponents of the multisite entanglement for large lattices tend to diverge for odd and even ladders, as the number of legs are increased, even though the amount of the multisite entanglement converges in the asymptotic limit. Wider implications . We believe that the results presented in the manuscript will be of interest to the broad physics community working on stronglycorrelated systems, quantum information in many-body physics, and related quantum technologies. The methodology presented in the manuscript will, we believe, also appeal to the general theoretical physics community.
We introduce an analytical iterative method, the density matrix recursion method, to generate arbitrary reduced density matrices of superpositions of short-range dimer coverings on periodic or non-periodic quantum spin-1/2 ladder lattices, with an arbitrary number of legs. The method can be used to calculate bipartite as well as multipartite physical properties, including bipartite and multi-partite entanglement. We apply this technique to distinguish between even- and odd-legged ladders. Specifically, we show that while genuine multi-partite entanglement decreases with increasing system size for the even-legged ladder states, it does the opposite for odd-legged ones.
The S=1/2 antiferromagnetic Heisenberg model on multi-leg ladders is investigated. Criticality of the ground-state transition is explored by means of finite-size scaling. The ladders with an even number of legs and those with an odd number of legs are distinguished clearly. In the former, the energy gap opens up as Delta E approximately J perpendicular to , where J perpendicular to is the strength of the antiferromagnetic inter-chain coupling. In the latter, the critical phase with the central charge c=1 extends over the whole region of J perpendicular to >0.
We investigate the NNN-leg spin-SSS Heisenberg ladders by using the density matrix renormalization group method. We present estimates of the spin gap ${\ensuremath{\Delta}}_{s}$ and of the ground-state energy per site ${e}_{\ensuremath{\infty}}^{N}$ in the thermodynamic limit for ladders with widths up to six legs and spin $S\ensuremath{\le}\frac{5}{2}$. We also estimate the ground-state energy per site ${e}_{\ensuremath{\infty}}^{2\mathrm{D}}$ for the infinite two-dimensional spin-SSS Heisenberg model. Our results support that for ladders with semi-integer spins the spin excitation is gapless for NNN odd and gapped for NNN even, whereas for integer spin ladders the spin gap is nonzero, independent of the number of legs. Those results agree with the well-known conjectures of Haldane and S\'en\'echal-Sierra for chains and ladders, respectively. We also observe edge states for ladders with NNN odd, similar to what happens in spin chains.
We present a density matrix renormalization group study of the ground-state properties of spin-1/2 frustrated J1-J3 Heisenberg n(l)-leg ladders (with n(l) up to 8). For strong frustration (J(3)/J(1) approximately 0.5), both even-leg and odd-leg ladders display a finite gap to spin excitations, which we argue remains finite in the two-dimensional limit. In this regime, on odd-leg ladders the ground state is spontaneously dimerized, in agreement with the Lieb-Schultz-Mattis prediction, while on even-leg ladders the dimer correlations decay exponentially. The magnitude of the dimer order parameter decreases as the number of legs increases, consistent with a two-dimensional spin-liquid ground state.
Motivated by near-term experiments with ultracold alkaline-earth atoms confined to optical lattices, we establish numerically and analytically the phase diagram of two-leg SU(N)\mathrm{SU}(N)SU(N) spin ladders. Two-leg ladders provide a rich and highly nontrivial extension of the single chain case on the way towards the relatively little explored two-dimensional situation. Focusing on the experimentally relevant limit of one fermion per site, antiferromagnetic exchange interactions, and $2\ensuremath{\le}N\ensuremath{\le}6$, we show that the phase diagrams as a function of the interchain (rung) to intrachain (leg) coupling ratio, ${J}_{\ensuremath{\perp}}/{J}_{\ensuremath{\parallel}}$, strongly differ for even versus odd NNN. For even N=4N=4N=4 and 6, we demonstrate that the phase diagram consists of a single valence bond crystal (VBC) with a spatial period of N/2N/2N/2 rungs. For odd N=3N=3N=3 and 5, we find surprisingly rich phase diagrams exhibiting three distinct phases. For weak rung coupling, we obtain a VBC with a spatial period of NNN rungs, whereas for strong coupling we obtain a critical phase related to the case of a single chain. In addition, we encounter intermediate phases for odd NNN, albeit of a different nature for N=3N=3N=3 as compared to N=5N=5N=5. For N=3N=3N=3, we find a novel gapless intermediate phase with ${J}_{\ensuremath{\perp}}$-dependent incommensurate spatial fluctuations in a sizeable region of the phase diagram. For N=5N=5N=5, there are strong indications for a narrow potentially gapped intermediate phase, whose nature is not entirely clear. Our results are based on (i) field theoretical techniques, (ii) qualitative symmetry considerations, and (iii) large-scale density matrix renormalization group (DMRG) simulations keeping beyond a million of states by fully exploiting and thus preserving the SU(N)\mathrm{SU}(N)SU(N) symmetry.
We devise a method based on the tensor-network formalism to calculate genuine multisite entanglement in ground states of infinite spin chains containing spin-1/2 or spin-1 quantum particles. The ground state is obtained by employing an infinite time-evolving block decimation method acting upon an initial matrix product state for the infinite spin system. We explicitly show how such infinite matrix product states with translational invariance provide a natural framework to derive the generalized geometric measure, a computable measure of genuine multisite entanglement, in the thermodynamic limit of quantum many-body systems with both spin-1/2 and higher-spin particles.