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Efekti konačne veličine u XY lancu

Vanja Marić

Published Jul 14, 2017• 0 citations
OpenAlex

Abstract

The XY chain in a transverse field is a prototypical exactly solvable model with interesting and desirable properties: its two-dimensional phase diagram, characterized by an anisotropy parameter and the strength of an external magnetic field, hosts two different quantum phase transitions at zero temperature, while the model can always be mapped into a system of free (spin-less) fermions. One of the phase transitions is the universality of free fermions (c = 1 CFT), while the other is that of the 1D quantum Ising model (c = 1=2 CFT). As a matter of fact, the XY chain is a generalization of the Ising chain. While both lines of phase transitions can be described by Conformal Field Theory, the bi-critical point at which these lines meet is non-conformal, since it has a quadratic spectrum. The aim of this thesis is to observe the non-conformal nature of the bi-critical point in the XY chain in a numerical experiment trough quantities accessible also in non-exactly solvable models, such as the entanglement entropy and the eigenvalues of the reduced density matrix. In this way, we want to propose in the future numerical tests whether a multi-critical point in an arbitrary model is conformal or not. First we introduce the XY chain and using standard analytical methods find its microscopic solution. Like the Ising model, the XY chain has a phase of broken Z2 symmetry, where the model shows two degenerate ground states in the thermodynamic limit of infinite system length. Having noticed a scarcity of results on the exact energy degeneracy between two putative ground states, we examine the problem using numerical and analytical methods. The analytical method, employing complex analysis and Fourier series, has given a definite answer for the Ising model. Using this method for the more general XY chain we find the dependence of the exact degeneracy on the number of spins in the special case of zero magnetic field and show the absence of an exact degeneracy when the anisotropy is greater than 1 and the number of spins is even. Coming back to the main aim of the thesis, we derive the reduced density matrix eigenvalues and the entanglement entropy in the XY chain and construct a numerical algorithm for calculating them. We accomplish to discriminate the non-conformal nature of the bi-critical point by comparing the entanglement entropy and the largest reduced density matrix eigenvalue with the conformal field theory predictions near and far from the bi-critical point.

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The XY chain in a transverse field is a prototypical exactly solvable model with interesting and desirable properties: its two-dimensional phase diagram, characterized by an anisotropy parameter and the strength of an external magnetic field, hosts two different quantum phase transitions at zero temperature, while the model can always be mapped into a system of free (spin-less) fermions. One of the phase transitions is the universality of free fermions (c = 1 CFT), while the other is that of the 1D quantum Ising model (c = 1=2 CFT). As a matter of fact, the XY chain is a generalization of the Ising chain. While both lines of phase transitions can be described by Conformal Field Theory, the bi-critical point at which these lines meet is non-conformal, since it has a quadratic spectrum. The aim of this thesis is to observe the non-conformal nature of the bi-critical point in the XY chain in a numerical experiment trough quantities accessible also in non-exactly solvable models, such as the entanglement entropy and the eigenvalues of the reduced density matrix. In this way, we want to propose in the future numerical tests whether a multi-critical point in an arbitrary model is conformal or not. First we introduce the XY chain and using standard analytical methods find its microscopic solution. Like the Ising model, the XY chain has a phase of broken Z2 symmetry, where the model shows two degenerate ground states in the thermodynamic limit of infinite system length. Having noticed a scarcity of results on the exact energy degeneracy between two putative ground states, we examine the problem using numerical and analytical methods. The analytical method, employing complex analysis and Fourier series, has given a definite answer for the Ising model. Using this method for the more general XY chain we find the dependence of the exact degeneracy on the number of spins in the special case of zero magnetic field and show the absence of an exact degeneracy when the anisotropy is greater than 1 and the number of spins is even. Coming back to the main aim of the thesis, we derive the reduced density matrix eigenvalues and the entanglement entropy in the XY chain and construct a numerical algorithm for calculating them. We accomplish to discriminate the non-conformal nature of the bi-critical point by comparing the entanglement entropy and the largest reduced density matrix eigenvalue with the conformal field theory predictions near and far from the bi-critical point.
The entanglement in quantum XY spin chains of arbitrary length is investigated via the geometric measure of entanglement. The emergence of entanglement is explained intuitively from the perspective of perturbations. The model is solved exactly and the energy spectrum is determined and analyzed in particular for the lowest two levels for both finite and infinite systems. The overlaps for these two levels are calculated analytically for arbitrary number of spins. The entanglement is hence obtained by maximizing over a single parameter. The corresponding ground-state entanglement surface is then determined over the entire phase diagram, and its behavior can be used to delineate the boundaries in the phase diagram. For example, the field-derivative of the entanglement becomes singular along the critical line. The form of the divergence is derived analytically and it turns out to be dictated by the universality class controlling the quantum phase transition. The behavior of the entanglement near criticality can be understood via a scaling hypothesis, analogous to that for free energies. The entanglement density vanishes along the so-called disorder line in the phase diagram, the ground space is doubly degenerate and spanned by two product states. The entanglement for the superposition of the lowest two states is also calculated. The exact value of the entanglement depends on the specific form of superposition. However, in the thermodynamic limit the entanglement density turns out to be independent of the superposition. This proves that the entanglement density is insensitive to whether the ground state is chosen to be the spontaneously Z2Z_2Z2​ symmetry broken one or not. The finite-size scaling of entanglement at critical points is also investigated from two different view points. First, the maximum in the field-derivative of the entanglement density is computed and fitted to a logarithmic dependence of the system size, thereby deducing the correlation length exponent for the Ising class using only the behavior of entanglement. Second, the entanglement density itself is shown to possess a correction term inversely proportional to the system size, with the coefficient being universal (but with different values for the ground state and the first excited state, respectively).
We study the R´enyi entropy and subsystem distances on one interval for the finite size and thermal states in the critical XY chains, focusing on the critical Ising chain and XX chain with zero transverse field. We construct numerically the reduced density matrices and calculate the von Neumann entropy, R´enyi entropy, subsystem trace distance, Schatten two-distance, and relative entropy. As the continuum limit of the critical Ising chain and XX chain with zero field are, respectively, the two-dimensional free massless Majorana and Dirac fermion theories, which are conformal field theories, we compare the spin chain numerical results with the analytical results in conformal field theories and find perfect matches in the continuum limit.
We calculate the entanglement and the universal boundary entropy (BE) in critical quantum spin chains, such as the transverse field Ising chain and the XXZ chain, with arbitrary direction of the boundary magnetic field (ADBMF). We determine the boundary universality class that an ADBMF induces. In particular, we show that the induced boundary conformal field theory depends on the point on the Bloch sphere where the boundary magnetic field directs. We show that the classification of the directions boils down to the simple fact that the boundary field breaks the bulk symmetry or does not. We present a procedure to estimate the universal BE, based on the finite-size corrections of the entanglement entropy, which apply to ADBMF. To calculate the universal BE in the XXZ chain, we use the density matrix renormalization group. The transverse field XY chain with ADBMF after Jordan-Wigner transformation is not a quadratic free fermion Hamiltonian. We map this model to a quadratic free fermion chain by introducing two extra ancillary spins coupled to the main chain at the boundaries, which makes the problem integrable. The eigenstates of the transverse field XY chain can be obtained by proper projection in the enlarged chain. Using this mapping, we are able to calculate the entanglement entropy of the transverse field XY chain using the usual correlation matrix technique up to relatively large sizes.
Abstract We study the Rényi entropy and subsystem distances on one interval for the finite size and thermal states in the critical XY chains, focusing on the critical Ising chain and XX chain with zero transverse field. We construct numerically the reduced density matrices and calculate the von Neumann entropy, Rényi entropy, subsystem trace distance, Schatten two-distance, and relative entropy. As the continuum limit of the critical Ising chain and XX chain with zero field are, respectively, the two-dimensional free massless Majorana and Dirac fermion theories, which are conformal field theories, we compare the spin chain numerical results with the analytical results in conformal field theories and find perfect matches in the continuum limit.
Abstract We calculate exactly the probability to find the ground state of the XY chain in a given spin configuration in the transverse σ z -basis. By determining finite-volume corrections to the probabilities for a wide variety of configurations, we obtain the universal boundary entropy at the critical point. The latter is a benchmark of the underlying boundary conformal field theory characterizing each quantum state. To determine the scaling of the probabilities, we prove a theorem that expresses, in a factorized form, the eigenvalues of a sub-matrix of a circulant matrix as functions of the eigenvalues of the original matrix. Finally, the boundary entropies are computed by exploiting a generalization of the Euler–MacLaurin formula to non-differentiable functions. It is shown that, in some cases, the spin configuration can flow to a linear superposition of Cardy states. Our methods and tools are rather generic and can be applied to all the periodic quantum chains which map to free-fermionic Hamiltonians.
In this thesis we have studied the emergence of spontaneously dimerized phases in frustrated spin-S chains, with emphasis on the nature of the critical lines between the dimerized and non-dimerized phases. The main numerical method used in this thesis is the Density Matrix Renormalization Group (DMRG). The DMRG algorithm is a relatively old and well established method for the investigation of the ground-state. In this thesis, we show how to use this algorithm to calculate the excitation spectra of one-dimensional critical systems, known in the context of conformal field theory as conformal towers of states. We have demonstrated that the method works very well for two simple minimal models (the transverse-field Ising model and the three-state Potts model), and we have used it systematically to identify the universality classes and the underlying conformal field theories of various one-dimensional spin systems. It has been known for a long time that the transition to a spontaneously dimerized phase in a spin-1 chain can be either continuous, in the Wess-Zumino-Witten (WZW) SU(2) level 2 universality class, or first order. By combining a careful numerical investigation with a conformal field theory analysis, we were able to detect in a frustrated spin-1 chain with competing next-nearest-neighbor and three-site interactions the presence of yet another type of continuous phase transition that belongs to the Ising universality class. In contrast to the WZW SU(2) level 2 critical line, at which the singlet-triplet gap closes, the Ising transition occurs entirely in the singlet sector, while the singlet-triplet gap remains open. The use of the standard DMRG approach, along the lines mentioned above, has allowed us to provide explicit numerical evidence for the presence of a conformal tower of singlets inside the spin gap. Moreover, according to field theory, a WZW SU(2) level k critical line can turn into a first order transition due to the presence of a marginal operator in the WZW SU(2) level k model. A careful investigation of the conformal towers along the critical lines has allowed us to find the precise location of this point in both S=1 and S=3/2 chains. We have also shown that the nature of the continuous dimerization transitions is related to the topological properties of the corresponding phases, and that the phase diagrams of various frustrated spin chains can be effectively extracted by looking at the local topological order parameter - the degeneracy of the lowest state in the entanglement spectrum. When coupled with the conformal field theory of open systems, DMRG appears to be an extremely powerful tool to characterize not only the phase diagram and the ground-state correlations of quantum one-dimensional systems, but also the excitation spectrum and the conformal structure along critical lines.