Publications (18)68.09 Total impact
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ABSTRACT: Recently, it was argued that the braiding and statistics of anyons in a twodimensional topological phase can be extracted by studying the quantum entanglement of the degenerate groundstates on the torus. This construction either required a lattice symmetry (such as $\pi/2$ rotation) or tacitly assumed that the `minimum entanglement states' (MESs) for two different bipartitions can be uniquely assigned quasiparticle labels. Here we describe a procedure to obtain the modular $\mathcal S$ matrix, which encodes the braiding statistics of anyons, which does not require making any of these assumptions. Our strategy is to compare MESs of three independent entanglement bipartitions of the torus, which leads to a unique modular $\mathcal S$. This procedure also puts strong constraints on the modular $\mathcal T$ matrix without requiring any symmetries, and in certain special cases, completely determines it. Our method applies equally to Abelian and nonAbelian topological phases.Physical Review B 12/2014; 91(3). DOI:10.1103/PhysRevB.91.035127 · 3.74 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: Quantum Spin Liquids (QSLs) are phases of interacting spins that do not order even at the absolute zero temperature, making it impossible to characterize them by a local order parameter. In this article, we review the unique view provided by the quantum entanglement on QSLs. We illustrate the crucial role of Topological Entanglement Entropy in diagnosing the nonlocal order in QSLs, using specific examples such as the Chiral Spin Liquid. We also demonstrate the detection of anyonic quasiparticles and their braiding statistics using quantum entanglement. In the context of gapless QSLs, we discuss the detection of emergent fermionic spinons in a bosonic wavefunction, by studying the size dependence of entanglement entropy.New Journal of Physics 02/2013; 15(2). DOI:10.1088/13672630/15/2/025002 · 3.56 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: We use entanglement entropy signatures to establish nonAbelian topological order in projected Cherninsulator wavefunctions. The simplest instance is obtained by Gutzwiller projecting a filled band with Chern number C=2, whose wavefunction may also be viewed as the square of the Slater determinant of a band insulator. We demonstrate that this wavefunction is captured by the $SU(2)_2$ Chern Simons theory coupled to fermions. This is established most persuasively by calculating the modular Smatrix from the candidate ground state wavefunctions, following a recent entanglement entropy based approach. This directly demonstrates the peculiar nonAbelian braiding statistics of Majorana fermion quasiparticles in this state. We also provide microscopic evidence for the field theoretic generalization, that the Nth power of a Chern number C Slater determinant realizes the topological order of the $SU(N)_C$ Chern Simons theory coupled to fermions, by studying the $SU(2)_3$ (ReadRezayi type state) and the $SU(3)_2$ wavefunctions. An advantage of our projected Chern insulator wavefunctions is the relative ease with which physical properties, such as entanglement entropy and modular Smatrix can be numerically calculated using Monte Carlo techniques.Physical review. B, Condensed matter 09/2012; 87(16). DOI:10.1103/PhysRevB.87.161113 · 3.66 Impact Factor  Physical review. B, Condensed matter 05/2012; 85(19). DOI:10.1103/PhysRevB.85.199905 · 3.66 Impact Factor
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ABSTRACT: Topologically ordered phases are gapped states, defined by the properties of excitations when taken around each other. By calculating Topological Entanglement Entropy (TEE) of a disc shaped partition using a Monte Carlo technique, we establish the existence of topological order in SU(2) symmetric gapped spin liquids and lattice Laughlin states obtained by the Gutzwiller projection technique. On the other hand, the TEE of partitioning the torus into two cylinders is generally different and depends on the chosen ground state. We demonstrate a method to extract the statistics and braiding of excitations, given just the set of ground state wavefunctions on a torus. Central to our scheme is the identification of groundstates with minimum entanglement entropy, which reflect the quasiparticle excitations. We demonstrate our method by extracting the modularS matrix of an SU(2) symmetric chiral spin liquid, and prove that its quasiparticles obey semionic statistics. This method offers a route to a nearly complete determination of the topological order in several cases.  [Show abstract] [Hide abstract]
ABSTRACT: Topologically ordered phases are gapped states, defined by the properties of excitations when taken around one another. Here we demonstrate a method to extract the statistics and braiding of excitations, given just the set of groundstate wave functions on a torus. This is achieved by studying the topological entanglement entropy (TEE) upon partitioning the torus into two cylinders. In this setting, general considerations dictate that the TEE generally differs from that in trivial partitions and depends on the chosen ground state. Central to our scheme is the identification of ground states with minimum entanglement entropy, which reflect the quasiparticle excitations of the topological phase. The transformation of these states allows for the determination of the modular S and U matrices which encode quasiparticle properties. We demonstrate our method by extracting the modular S matrix of a chiral spin liquid phase using a Monte Carlo scheme to calculate the TEE and prove that the quasiparticles obey semionic statistics. This method offers a route to nearly complete determination of the topological order in certain cases.Physical review. B, Condensed matter 11/2011; 85(23). DOI:10.1103/PhysRevB.85.235151 · 3.66 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: Quantum spin liquids are phases of matter whose internal structure is not captured by a local order parameter. Particularly intriguing are critical spin liquids, where strongly interacting excitations control low energy properties. Here we calculate their bipartite entanglement entropy that characterizes their quantum structure. In particular we calculate the Renyi entropy S(2) on model wave functions obtained by Gutzwiller projection of a Fermi sea. Although the wave functions are not sign positive, S(2) can be calculated on relatively large systems (>324 spins) using the variational Monte Carlo technique. On the triangular lattice we find that entanglement entropy of the projected Fermi sea state violates the boundary law, with S(2) enhanced by a logarithmic factor. This is an unusual result for a bosonic wave function reflecting the presence of emergent fermions. These techniques can be extended to study a wide class of other phases.Physical Review Letters 08/2011; 107(6):067202. DOI:10.1103/PhysRevLett.107.067202 · 7.51 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: We study entanglement properties of candidate wavefunctions for SU(2) symmetric gapped spin liquids and Laughlin states. These wavefunctions are obtained by the Gutzwiller projection technique. Using Topological Entanglement Entropy \gamma\ as a tool, we establish topological order in chiral spin liquid and Z2 spin liquid wavefunctions, as well as a lattice version of the Laughlin state. Our results agree very well with the field theoretic result \gamma =log D where D is the total quantum dimension of the phase. All calculations are done using a Monte Carlo technique on a 12 times 12 lattice enabling us to extract \gamma\ with small finite size effects. For a chiral spin liquid wavefunction, the calculated value is within 4% of the ideal value. We also find good agreement for a lattice version of the Laughlin \nu =1/3 phase with the expected \gamma=log \sqrt{3}.Physical review. B, Condensed matter 05/2011; 84(7). DOI:10.1103/PhysRevB.84.075128 · 3.66 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: There are many phases of insulators with inversion symmetry (with no other symmetry required). In particular, certain inversion parities cannot change unless there is a phase transition. I will show how to use these parities to classify phases of topological insulators and explain which combinations of these parities have physical consequences (e.g. for the magnetoelectric effect). Many of these results can be derived by pictorial arguments using the entanglement spectrum.  [Show abstract] [Hide abstract]
ABSTRACT: Spin liquids are exotic quantum states that do not break any symmetry. Though much is known about gapped spinliquids, critical spinliquids with strongly interacting gapless excitations in two and three spatial dimensions are less understood. Candidate ground state wavefunctions for such states however can be constructed using the Gutzwiller projection method. We use bipartite entanglement entropy, in particular the Renyi entropy S2 to investigate the quantum structure of these wavefunctions. Using the Variational MonteCarlo technique, we calculate the Renyi entropy of a critical spin liquid  the projected Fermi sea state on the triangular lattice. We find a violation of the boundary law, with S2 enhanced by a logarithmic factor, an unusual result for a bosonic wavefunction reflecting the presence of emergent spinons that form a Fermi surface. The Renyi entropy for algebraic spin liquids is found to obey the area law, consistent with the presence of emergent Dirac fermions in the system. Projection is found to completely alter the entanglement properties of nested Fermi surface states. These results show that the Renyi entropy calculations could serve as a diagnostic for gapless fractionalized phases.  [Show abstract] [Hide abstract]
ABSTRACT: Topological band insulators are usually characterized by symmetryprotected surface modes or quantized linearresponse functions (like Hall conductance). Here we present a way to characterize them based on certain bulk properties of just the groundstate wave function, specifically, the properties of its entanglement spectrum. We prove that whenever protected surface states exist, a corresponding protected “mode” exists in the entanglement spectrum as well. Besides this, the entanglement spectrum sometimes succeeds better at indicating topological phases than surface states. We discuss specifically the example of insulators with inversion symmetry which is found to act as an antiunitary symmetry on the entanglement spectrum. A Kramers degeneracy can then arise even when timereversal symmetry is absent. This degeneracy persists for interacting systems. The entanglement spectrum is therefore a promising tool to characterize topological band insulators and superconductors beyond the freeparticle approximation.Physical review. B, Condensed matter 12/2010; 82(24). DOI:10.1103/PhysRevB.82.241102 · 3.66 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: We study AharonovBohm (AB) conductance oscillations arising from the surface states of a topological insulator nanowire, when a magnetic field is applied along its length. With strong surface disorder, these oscillations are predicted to have a component with anomalous period Φ(0)=hc/e, twice the conventional period. The conductance maxima are achieved at odd multiples of 1/2Φ(0), implying that a π AB phase for electrons strengthens the metallic nature of surface states. This effect is special to topological insulators, and serves as a defining transport property. A key ingredient, the surface curvature induced Berry phase, is emphasized here. We discuss similarities and differences from recent experiments on Bi2Se3 nanoribbons, and optimal conditions for observing this effect.Physical Review Letters 11/2010; 105(20):206601. DOI:10.1103/PhysRevLett.105.206601 · 7.51 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: We study three dimensional insulators with inversion symmetry, in which other point group symmetries, such as time reversal, are generically absent. Their band topology is found to be classified by the parities of occupied states at time reversal invariant momenta (TRIM parities), and by three Chern numbers. The TRIM parities of any insulator must satisfy a constraint: their product must be +1. The TRIM parities also constrain the Chern numbers modulo two. When the Chern numbers vanish, a magnetoelectric response parameterized by "theta" is defined and is quantized to theta= 0, 2pi. Its value is entirely determined by the TRIM parities. These results may be useful in the search for magnetic topological insulators with large theta. A classification of inversion symmetric insulators is also given for general dimensions. An alternate geometrical derivation of our results is obtained by using the entanglement spectrum of the ground state wavefunction.Physical review. B, Condensed matter 10/2010; 85(16). DOI:10.1103/PhysRevB.85.165120 · 3.66 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: Dislocations in topological insulators can host a onedimensional metallic state that is topologically protected. We discuss experimental consequences for Bi0.9Sb0.1 alloys, including an unusual straininduced conductivity effect. With a view to studying interaction effects, microscopic parameters for the onedimensional metallic modes are derived, starting from a LiuAllen tightbinding model. The Luttinger parameter for the onedimensional metal in Bi0.9Sb0.1 is estimated. A different route to a metallic defect line is found in model systems where SU(2) spin rotation symmetry is spontaneously broken, leading to a topological insulator. Line defects of the order parameter are found to be metallic, if a strong topological insulator is realized. We study models exhibiting this phase on the diamond and ideal wurtzite lattices. Prospects for experimental realizations are discussed.  [Show abstract] [Hide abstract]
ABSTRACT: How do we uniquely identify a quantum phase, given its ground state wavefunction? This is a key question for many body theory especially when we consider phases like topological insulators, that share the same symmetry but differ at the level of topology. The entanglement spectrum has been proposed as a ground state property that captures characteristic edge excitations. Here we study the entanglement spectrum for topological band insulators. We first show that insulators with topological surface states will necessarily also have protected modes in the entanglement spectrum. Surprisingly, however, the converse is not true. Protected entanglement modes can also appear for insulators without physical surface states, in which case they capture a more elusive property. This is illustrated by considering insulators with only inversion symmetry. Inversion is shown to act in an unusual way, as an antiunitary operator, on the entanglement spectrum, leading to this protection. The entanglement degeneracies indicate a variety of different phases in inversion symmetric insulators, and these phases are argued to be robust to the introduction of interactions.  [Show abstract] [Hide abstract]
ABSTRACT: We study three dimensional systems where strong repulsion leads to an insulating state via spontaneously generated spinorbit interactions. We discuss a microscopic model where the resulting state is topological. Such topological `Mott' insulators differ from their band insulator counterparts in that they possess an additional order parameter, a rotation matrix, that describes the spontaneous breaking of spinrotation symmetry. We show that line defects of this order are associated with protected one dimensional modes in the {\em strong} topological Mott insulator, which provides a bulk characterization of this phase.Physical review. B, Condensed matter 04/2009; 79(24). DOI:10.1103/PhysRevB.79.245331 · 3.66 Impact Factor 
Article: Onedimensional topologically protected modes in topological insulators with lattice dislocations
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ABSTRACT: Topological defects, such as domain walls and vortices, have long fascinated physicists. A novel twist is added in quantum systems such as the Bphase of superfluid helium He3, where vortices are associated with lowenergy excitations in the cores. Similarly, cosmic strings may be tied to propagating fermion modes. Can analogous phenomena occur in crystalline solids that host a plethora of topological defects? Here, we show that indeed dislocation lines are associated with onedimensional fermionic excitations in a `topological insulator', a novel phase of matter believed to be realized in the material Bi0.9Sb0.1. In contrast to fermionic excitations in a regular quantum wire, these modes are topologically protected and not scattered by disorder. As dislocations are ubiquitous in real materials, these excitations could dominate spin and charge transport in topological insulators. Our results provide a novel route to creating a potentially ideal quantum wire in a bulk solid.Nature Physics 03/2009; 5(4):298303. DOI:10.1038/nphys1220 · 20.15 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: Topological defects, such as domain walls and vortices, have long fascinated physicists. A novel twist is added in quantum systems like the Bphase of superfluid helium He$_3$, where vortices are associated with low energy excitations in the cores. Similarly, cosmic strings may be tied to propagating fermion modes. Can analogous phenomena occur in crystalline solids that host a plethora of topological defects? Here we show that indeed dislocation lines are associated with one dimensional fermionic excitations in a `topological insulator', a novel band insulator believed to be realized in the bulk material Bi$_{0.9}$Sb$_{0.1}$. In contrast to fermionic excitations in a regular quantum wire, these modes are topologically protected like the helical edge states of the quantum spinHall insulator, and not scattered by disorder. Since dislocations are ubiquitous in real materials, these excitations could dominate spin and charge transport in topological insulators. Our results provide a novel route to creating a potentially ideal quantum wire in a bulk solid.
Publication Stats
577  Citations  
68.09  Total Impact Points  
Top Journals
Institutions

2014

Stanford University
 Department of Physics
Palo Alto, California, United States


2013

University of California, Santa Barbara
 Kavli Institute for Theoretical Physics
Santa Barbara, California, United States


20092012

University of California, Berkeley
 Department of Physics
Berkeley, California, United States
