2010
DOI: 10.1103/physrevb.81.064439
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Entanglement spectrum of a topological phase in one dimension

Abstract: We show that the Haldane phase of S=1 chains is characterized by a double degeneracy of the entanglement spectrum. The degeneracy is protected by a set of symmetries (either the dihedral group of $\pi$-rotations about two orthogonal axes, time-reversal symmetry, or bond centered inversion symmetry), and cannot be lifted unless either a phase boundary to another, "topologically trivial", phase is crossed, or the symmetry is broken. More generally, these results offer a scheme to classify gapped phases of one di… Show more

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Cited by 1,226 publications
(1,753 citation statements)
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“…Following established techniques [116][117][118], let U I denote the action of inversion and U θ ↑/↓ the U(1) symmetries of the upper/lower layer when acting on Schmidt states. A priori, these U have U(1) phase ambiguities, which we will gauge fix as follows.…”
Section: Spin-charge Separationmentioning
confidence: 99%
“…Following established techniques [116][117][118], let U I denote the action of inversion and U θ ↑/↓ the U(1) symmetries of the upper/lower layer when acting on Schmidt states. A priori, these U have U(1) phase ambiguities, which we will gauge fix as follows.…”
Section: Spin-charge Separationmentioning
confidence: 99%
“…That is, two time-reversal twists compose into identity up to a universal phase factor characterizing the underlying SPT order of the state. In 1D, the distinction between different time-reversal SPT phases has been well understood in the matrix product formalism [ [17][18][19][20]. Our discussion is just a reinterpretation of that procedure in terms of local time-reversal symmetry action and time-reversal twists.…”
Section: Introductionmentioning
confidence: 99%
“…II, we discuss the 1D case in terms of matrix product states (MPS) and present a way to insert timereversal fluxes through a 1D ring. In 1D there are two different time-reversal symmetry-protected topological phases [16][17][18]. We demonstrate how these two phases can be distinguished from each other using the projective composition rule of time-reversal twists induced by the inserted time-reversal fluxes.…”
Section: Introductionmentioning
confidence: 99%
“…This non-trivial property is protected by symmetry, because once the symmetry is removed, the SPT phases can be smoothly connected to the trivial phase without phase transitions. 3 The well known Haldane phase 4 is an example of SPT phase in 1-dimension (1D). Topological insulators [5][6][7][8][9][10] are examples of SPT phases in higher dimensions.…”
Section: Introductionmentioning
confidence: 99%