0000000000380648

AUTHOR

Augustine Kshetrimayum

showing 5 related works from this author

The classical two-dimensional Heisenberg model revisited: An $SU(2)$-symmetric tensor network study

2021

The classical Heisenberg model in two spatial dimensions constitutes one of the most paradigmatic spin models, taking an important role in statistical and condensed matter physics to understand magnetism. Still, despite its paradigmatic character and the widely accepted ban of a (continuous) spontaneous symmetry breaking, controversies remain whether the model exhibits a phase transition at finite temperature. Importantly, the model can be interpreted as a lattice discretization of the $O(3)$ non-linear sigma model in $1+1$ dimensions, one of the simplest quantum field theories encompassing crucial features of celebrated higher-dimensional ones (like quantum chromodynamics in $3+1$ dimensio…

Sigma modelSpontaneous symmetry breakingQC1-999Lattice (group)General Physics and AstronomyFOS: Physical sciencesClassical Heisenberg modelQuantum Materials53001 natural sciences010305 fluids & plasmasTheoretical physicsHigh Energy Physics - Lattice0103 physical sciencesSymmetric tensorTensorQuantum field theory010306 general physicsclassical Heisenberg modelCondensed Matter - Statistical MechanicsPhysicsQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)Heisenberg modelPhysics500 Naturwissenschaften und Mathematik::530 Physik::530 PhysikHigh Energy Physics - Lattice (hep-lat)magnetismstatistical and condensed matter physicsQuantum Physics (quant-ph)
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Tensor Network Annealing Algorithm for Two-Dimensional Thermal States

2019

Tensor network methods have become a powerful class of tools to capture strongly correlated matter, but methods to capture the experimentally ubiquitous family of models at finite temperature beyond one spatial dimension are largely lacking. We introduce a tensor network algorithm able to simulate thermal states of two-dimensional quantum lattice systems in the thermodynamic limit. The method develops instances of projected entangled pair states and projected entangled pair operators for this purpose. It is the key feature of this algorithm to resemble the cooling down of the system from an infinite temperature state until it reaches the desired finite-temperature regime. As a benchmark we …

PhysicsOptical latticeQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)General Physics and AstronomyQuantum simulatortensor network methodsFOS: Physical sciences01 natural sciencesSquare latticequantum statistical mechanicsCondensed Matter - Strongly Correlated ElectronsExact solutions in general relativityquantum information0103 physical sciencesThermodynamic limit539strongly correlated systemsIsing modelQuantum information010306 general physicsQuantum statistical mechanicsQuantum Physics (quant-ph)Algorithmquantum simulationPhysical Review Letters
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Symmetry-protected intermediate trivial phases in quantum spin chains

2015

Symmetry-protected trivial (SPt) phases of matter are the product-state analogue of symmetry-protected topological (SPT) phases. This means, SPt phases can be adiabatically connected to a product state by some path that preserves the protecting symmetry. Moreover, SPt and SPT phases can be adiabatically connected to each other when interaction terms that break the symmetries protecting the SPT order are added in the Hamiltonian. It is also known that spin-1 SPT phases in quantum spin chains can emerge as effective intermediate phases of spin-2 Hamiltonians. In this paper we show that a similar scenario is also valid for SPt phases. More precisely, we show that for a given spin-2 quantum cha…

Quantum phase transitionPhysicsQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)Time-evolving block decimationFOS: Physical sciences02 engineering and technologyQuantum entanglementQuantum phasesAstrophysics::Cosmology and Extragalactic Astrophysics021001 nanoscience & nanotechnology01 natural sciencesCondensed Matter - Strongly Correlated ElectronsQuantum mechanics0103 physical sciencesThermodynamic limitTopological order010306 general physics0210 nano-technologyCentral chargeQuantum Physics (quant-ph)Phase diagram
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The spin-1/2 Kagome XXZ model in a field: competition between lattice nematic and solid orders

2016

We study numerically the spin-1/2 XXZ model in a field on an infinite Kagome lattice. We use different algorithms based on infinite Projected Entangled Pair States (iPEPS) for this, namely: (i) with simplex tensors and 9-site unit cell, and (ii) coarse-graining three spins in the Kagome lattice and mapping it to a square-lattice model with nearest-neighbor interactions, with usual PEPS tensors, 6- and 12-site unit cells. Similarly to our previous calculation at the SU(2)-symmetric point (Heisenberg Hamiltonian), for any anisotropy from the Ising limit to the XY limit, we also observe the emergence of magnetization plateaus as a function of the magnetic field, at $m_z = \frac{1}{3}$ using 6-…

FOS: Physical sciences02 engineering and technology01 natural sciencesCondensed Matter - Strongly Correlated Electronssymbols.namesakeMagnetizationHigh Energy Physics - LatticeLattice (order)Quantum mechanics0103 physical sciencesTensor010306 general physicsComputingMilieux_MISCELLANEOUSPhysicsQuantum PhysicsSimplexStrongly Correlated Electrons (cond-mat.str-el)Degenerate energy levelsHigh Energy Physics - Lattice (hep-lat)021001 nanoscience & nanotechnologysymbolsIsing modelQuantum spin liquid[PHYS.COND.CM-SCE]Physics [physics]/Condensed Matter [cond-mat]/Strongly Correlated Electrons [cond-mat.str-el]0210 nano-technologyHamiltonian (quantum mechanics)Quantum Physics (quant-ph)
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All spin-1 topological phases in a single spin-2 chain

2014

Here we study the emergence of different Symmetry-Protected Topological (SPT) phases in a spin-2 quantum chain. We consider a Heisenberg-like model with bilinear, biquadratic, bicubic, and biquartic nearest-neighbor interactions, as well as uniaxial anisotropy. We show that this model contains four different effective spin-1 SPT phases, corresponding to different representations of the $(\mathbb{Z}_2 \times \mathbb{Z}_2) + T$ symmetry group, where $\mathbb{Z}_2$ is some $\pi$-rotation in the spin internal space and $T$ is time-reversal. One of these phases is equivalent to the usual spin-1 Haldane phase, while the other three are different but also typical of spin-1 systems. The model also …

Quantum phase transitionPhysicsStrongly Correlated Electrons (cond-mat.str-el)Conformal field theoryFOS: Physical sciencesFermionSymmetry groupCondensed Matter PhysicsTopologyElectronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated ElectronsQuantum mechanicsThermodynamic limitEffective field theoryCondensed Matter::Strongly Correlated ElectronsSpin (physics)Ground state
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