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Exactly solvable pairing model with p+ip wave symmetry

Miguel Ibáñez-Berganza, Jon Links, Germán Sierra, Shao-you Zhao A

Published Oct 2, 2008• 0 citations
OpenAlex

Abstract

We present the exact Bethe ansatz solution for the two-dimensional BCS pairing Hamiltonian with p_x + i p_y symmetry. Using both mean-field theory and the exact solution we obtain the ground-state phase diagram parameterized by the filling fraction and the coupling constant. It consists of three phases denoted weak coupling BCS, weak pairing, and strong pairing. The first two phases are separated by a topologically protected line where the exact ground state is given by the Moore-Read pfaffian state. In the thermodynamic limit the ground-state energy is discontinuous on this line. The other two phases are separated by the critical line, also topologically protected, previously found by Read and Green. We establish a duality relation between the weak and strong pairing phases, whereby ground states of the weak phase are dressed versions of the ground states of the strong phase by zero energy (Moore-Read) pairs and characterized by a topological order parameter.

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Exactly solvable pairing model for superconductors with px+ipy -wave symmetry

Miguel Ibáñez-Berganza, Jon Links, Germán Sierra +1 more

We present the exact Bethe ansatz solution for the two-dimensional BCS pairing Hamiltonian with ${p}_{x}+i{p}_{y}$ symmetry. Using both mean-field theory and the exact solution we obtain the ground-state phase diagram parametrized by the filling fraction and the coupling constant. It consists of three phases that are denoted weak-coupling BCS, weak pairing, and strong pairing. The first two phases are separated by a topologically protected line where the exact ground state is given by the Moore-Read pfaffian state. In the thermodynamic limit the ground-state energy is discontinuous on this line. The other two phases are separated by the critical line, also topologically protected, previously found by Read and Green. We establish a duality relation between the weak and strong pairing phases, whereby ground states of the weak phase are ``dressed'' versions of the ground states of the strong phase by zero energy (Moore-Read) pairs and characterized by a topological order parameter.

arXiv:0810.0340•Physical Review B•May 1, 2009•80 citations

Exact solution of the p + ip pairing Hamiltonian and a hierarchy of integrable models

Clare Dunning, Miguel Ibáñez-Berganza, Jon Links +2 more

Using the well-known trigonometric six-vertex solution of the Yang-Baxter equation we derive an integrable pairing Hamiltonian with anyonic degrees of freedom. The exact algebraic Bethe ansatz solution is obtained using standard techniques. From this model we obtain several limiting models, including the pairing Hamiltonian with p+ip-wave symmetry. An in-depth study of the p+ip model is then undertaken, including a mean-field analysis, analytic and numerical solution of the Bethe ansatz equations, and an investigation of the topological properties of the ground-state wavefunction. Our main result is that the ground-state phase diagram of the p+ip model consists of three phases. There is the known boundary line with gapless excitations that occurs for vanishing chemical potential, separating the topologically trivial strong pairing phase and the topologically non-trivial weak pairing phase. We argue that a second boundary line exists separating the weak pairing phase from a topologically trivial weak coupling BCS phase, which includes the Fermi sea in the limit of zero coupling. The ground state on this second boundary line is the Moore-Read state.

arXiv:1001.1591•Journal of Statistical Mechanics Theory and Experiment•Aug 26, 2010•57 citations

Bethe Ansatz analysis of the open and closed p + ip-pairing BCS models

Yibing Shen

The p+ip-wave pairing BCS model has attracted much attention due to its potential applications inexperimental physics, and the developing theory of topological superconductors. In this thesis, weinvestigate the p + ip BCS model as an integrable model with exact Bethe Ansatz solutions. Theground-state energies of this model will be studied with various methods.  First a brief introduction on quantum integrability is given, followed by an introduction to theQuantum Inverse Scattering Method, algebraic Bethe Ansatz and BCS theory of superconductivity. Wethen introduce a two-dimensional BCS pairing Hamiltonian with px +ipy symmetry. In the frameworkof the Quantum Inverse Scattering Method, the p+ip Hamiltonian can be constructed from a specificsolution of the non-standard classical Yang-Baxter equation. This solution produces a family ofconserved operators satisfying quadratic relations. Remarks on topological superconductivity for thep+ip-wave pairing model are provided.  We move on to investigate methods for calculating the ground-state energy for the p+ip Hamil-tonian. We first consider the Hamiltonian isolated from its environment (closed model) through twoforms of Bethe Ansatz solution, which generally have complex-valued Bethe roots. A continuum limitapproximation, leading to an integral equation, is applied to compute the ground-state energy. Theevolution of the root distribution curve with respect to a range of parameters is presented, followed bya discussion of the limitations of this method. Despite the limitations, the ground-state energy andthe ‘gap’ equation derived from the integral approximation are consistent with mean-field results fromprevious study.  We then consider the Hamiltonian interacting with its environment (open model) and begin witha mean-field analysis. We discuss the relation between the Bethe roots and the conserved operatoreigenvalues. The Bethe Ansatz solution of the open model is studied numerically, revealing complicatedbehaviour of the Bethe roots without a clear indication for an integral approximation.  Next we consider an alternative approach based on the quadratic relations among the real-valuedconserved operator eigenvalues. An integral equation is first established for the closed model. Thisequation is shown to admit an exact solution associated with the ground state.  Finally we extend the aforementioned alternative approach to the open model. Combined withresults from mean-field analysis, we are able to establish an integral equation with an exact solutionthat corresponds to the ground state for the open case.

•Sep 27, 2019•0 citations

Read-Green resonances in a $p_x+ip_y$ superfluid interacting with a bath

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We study the weak-pairing phase in a finite-size two-dimensional $p_x+ip_y$ superfluid interacting with an environment. This interaction breaks particle-number symmetry and can be modelled by means of an integrable Hamiltonian. We present the exact wave function and solve the resulting Bethe ansatz equations, from which it is shown how resonances are introduced at fixed interaction strengths. These cannot be observed within mean-field theory and are argued to be caused by zero-energy excitations at topologically protected Read-Green points.

•Jan 15, 2016•0 citations

Exact solution of the px+ipy pairing Hamiltonian by deforming the pairing algebra

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Recently, interest has increased in the hyperbolic family of integrable Richardson-Gaudin (RG) models. It was pointed out that a particular linear combination of the integrals of motion of the hyperbolic RG model leads to a Hamiltonian that describes $p$-wave pairing in a two-dimensional system. Such an interaction is found to be present in fermionic superfluids (${}^{3}\text{He}$), ultracold atomic gases, and $p$-wave superconductivity. Furthermore the phase diagram is intriguing, with the presence of the Moore-Read and Read-Green lines. At the Read-Green line a rare third-order quantum phase transition occurs. The present paper makes a connection between collective bosonic states and the exact solutions of the ${p}_{x}+i{p}_{y}$ pairing Hamiltonian. This makes it possible to investigate the effects of the Pauli principle on the energy spectrum, by gradually reintroducing the Pauli principle. It also introduces an efficient and stable numerical method to probe all the eigenstates of this class of Hamiltonians. We extend the phase diagram to repulsive interactions, an area that was not previously explored due to the lack of a proper mean-field solution in this region. We found a connection between the point in the phase diagram where the ground state connects to the bosonic state with the highest collectivity, and the Moore-Read line where all the Richardson-Gaudin (RG) variables collapse to zero. In contrast with the reduced BCS case, the overlap between the ground state and the highest collective state at the Moore-Read line is not the largest. In fact it shows a minimum when most other bosonic states show a maximum of the overlap. We found remnants of the Read-Green line for finite systems, by investigating the total spectrum. A symmetry was found between the Hamiltonian with and without single-particle part. When the interaction was repulsive we found four different classes of trajectories of the RG variables.

arXiv:1402.0339•Physical Review B•Apr 28, 2014•42 citations

An exactly soluble model with tunable p -wave paired fermion ground states

Yue Yu, Ziqiang Wang

Motivated by the work of Kitaev, we construct an exactly soluble spin-½ model on a honeycomb lattice whose ground states are identical to Δ 1 x p x +Δ 1 y p y + i (Δ 2 x p x +Δ 2 y p y )-wave paired fermions on a square lattice, with tunable paring order parameters. We derive a universal phase diagram for this general p -wave theory which contains a gapped A-phase and a topologically non-trivial B-phase. We show that the gapless condition in the B-phase is governed by a generalized inversion (G-inversion) symmetry under p x ↔ (Δ 1 y / Δ 1 x ) p y . The G-inversion symmetric gapless B-phase near the phase boundaries is described by (1+1)-dimensional gapless Majorana fermions in the asymptotic long-wavelength limit, i.e. the c =1/2 conformal field theory. The gapped B-phase has G-inversion symmetry breaking and is the weak pairing phase described by the Moore-Read Pfaffian. We show that in the gapped B-phase, vortex pair excitations are separated from the ground state by a finite energy gap.

arXiv:0708.0631•Europhysics Letters (EPL)•Nov 25, 2008•24 citations
We present the exact Bethe ansatz solution for the two-dimensional BCS pairing Hamiltonian with p_x + i p_y symmetry. Using both mean-field theory and the exact solution we obtain the ground-state phase diagram parameterized by the filling fraction and the coupling constant. It consists of three phases denoted weak coupling BCS, weak pairing, and strong pairing. The first two phases are separated by a topologically protected line where the exact ground state is given by the Moore-Read pfaffian state. In the thermodynamic limit the ground-state energy is discontinuous on this line. The other two phases are separated by the critical line, also topologically protected, previously found by Read and Green. We establish a duality relation between the weak and strong pairing phases, whereby ground states of the weak phase are dressed versions of the ground states of the strong phase by zero energy (Moore-Read) pairs and characterized by a topological order parameter.
We present the exact Bethe ansatz solution for the two-dimensional BCS pairing Hamiltonian with px+ipy{p}_{x}+i{p}_{y}px​+ipy​ symmetry. Using both mean-field theory and the exact solution we obtain the ground-state phase diagram parametrized by the filling fraction and the coupling constant. It consists of three phases that are denoted weak-coupling BCS, weak pairing, and strong pairing. The first two phases are separated by a topologically protected line where the exact ground state is given by the Moore-Read pfaffian state. In the thermodynamic limit the ground-state energy is discontinuous on this line. The other two phases are separated by the critical line, also topologically protected, previously found by Read and Green. We establish a duality relation between the weak and strong pairing phases, whereby ground states of the weak phase are ``dressed'' versions of the ground states of the strong phase by zero energy (Moore-Read) pairs and characterized by a topological order parameter.
Using the well-known trigonometric six-vertex solution of the Yang-Baxter equation we derive an integrable pairing Hamiltonian with anyonic degrees of freedom. The exact algebraic Bethe ansatz solution is obtained using standard techniques. From this model we obtain several limiting models, including the pairing Hamiltonian with p+ip-wave symmetry. An in-depth study of the p+ip model is then undertaken, including a mean-field analysis, analytic and numerical solution of the Bethe ansatz equations, and an investigation of the topological properties of the ground-state wavefunction. Our main result is that the ground-state phase diagram of the p+ip model consists of three phases. There is the known boundary line with gapless excitations that occurs for vanishing chemical potential, separating the topologically trivial strong pairing phase and the topologically non-trivial weak pairing phase. We argue that a second boundary line exists separating the weak pairing phase from a topologically trivial weak coupling BCS phase, which includes the Fermi sea in the limit of zero coupling. The ground state on this second boundary line is the Moore-Read state.
The p+ip-wave pairing BCS model has attracted much attention due to its potential applications inexperimental physics, and the developing theory of topological superconductors. In this thesis, weinvestigate the p + ip BCS model as an integrable model with exact Bethe Ansatz solutions. Theground-state energies of this model will be studied with various methods.  First a brief introduction on quantum integrability is given, followed by an introduction to theQuantum Inverse Scattering Method, algebraic Bethe Ansatz and BCS theory of superconductivity. Wethen introduce a two-dimensional BCS pairing Hamiltonian with px +ipy symmetry. In the frameworkof the Quantum Inverse Scattering Method, the p+ip Hamiltonian can be constructed from a specificsolution of the non-standard classical Yang-Baxter equation. This solution produces a family ofconserved operators satisfying quadratic relations. Remarks on topological superconductivity for thep+ip-wave pairing model are provided.  We move on to investigate methods for calculating the ground-state energy for the p+ip Hamil-tonian. We first consider the Hamiltonian isolated from its environment (closed model) through twoforms of Bethe Ansatz solution, which generally have complex-valued Bethe roots. A continuum limitapproximation, leading to an integral equation, is applied to compute the ground-state energy. Theevolution of the root distribution curve with respect to a range of parameters is presented, followed bya discussion of the limitations of this method. Despite the limitations, the ground-state energy andthe ‘gap’ equation derived from the integral approximation are consistent with mean-field results fromprevious study.  We then consider the Hamiltonian interacting with its environment (open model) and begin witha mean-field analysis. We discuss the relation between the Bethe roots and the conserved operatoreigenvalues. The Bethe Ansatz solution of the open model is studied numerically, revealing complicatedbehaviour of the Bethe roots without a clear indication for an integral approximation.  Next we consider an alternative approach based on the quadratic relations among the real-valuedconserved operator eigenvalues. An integral equation is first established for the closed model. Thisequation is shown to admit an exact solution associated with the ground state.  Finally we extend the aforementioned alternative approach to the open model. Combined withresults from mean-field analysis, we are able to establish an integral equation with an exact solutionthat corresponds to the ground state for the open case.
Read-Green resonances in a px+ipyp_x+ip_ypx​+ipy​ superfluid interacting with a bath
We study the weak-pairing phase in a finite-size two-dimensional px+ipyp_x+ip_ypx​+ipy​ superfluid interacting with an environment. This interaction breaks particle-number symmetry and can be modelled by means of an integrable Hamiltonian. We present the exact wave function and solve the resulting Bethe ansatz equations, from which it is shown how resonances are introduced at fixed interaction strengths. These cannot be observed within mean-field theory and are argued to be caused by zero-energy excitations at topologically protected Read-Green points.
Recently, interest has increased in the hyperbolic family of integrable Richardson-Gaudin (RG) models. It was pointed out that a particular linear combination of the integrals of motion of the hyperbolic RG model leads to a Hamiltonian that describes ppp-wave pairing in a two-dimensional system. Such an interaction is found to be present in fermionic superfluids (3He{}^{3}\text{He}3He), ultracold atomic gases, and ppp-wave superconductivity. Furthermore the phase diagram is intriguing, with the presence of the Moore-Read and Read-Green lines. At the Read-Green line a rare third-order quantum phase transition occurs. The present paper makes a connection between collective bosonic states and the exact solutions of the px+ipy{p}_{x}+i{p}_{y}px​+ipy​ pairing Hamiltonian. This makes it possible to investigate the effects of the Pauli principle on the energy spectrum, by gradually reintroducing the Pauli principle. It also introduces an efficient and stable numerical method to probe all the eigenstates of this class of Hamiltonians. We extend the phase diagram to repulsive interactions, an area that was not previously explored due to the lack of a proper mean-field solution in this region. We found a connection between the point in the phase diagram where the ground state connects to the bosonic state with the highest collectivity, and the Moore-Read line where all the Richardson-Gaudin (RG) variables collapse to zero. In contrast with the reduced BCS case, the overlap between the ground state and the highest collective state at the Moore-Read line is not the largest. In fact it shows a minimum when most other bosonic states show a maximum of the overlap. We found remnants of the Read-Green line for finite systems, by investigating the total spectrum. A symmetry was found between the Hamiltonian with and without single-particle part. When the interaction was repulsive we found four different classes of trajectories of the RG variables.
Motivated by the work of Kitaev, we construct an exactly soluble spin-½ model on a honeycomb lattice whose ground states are identical to Δ 1 x p x +Δ 1 y p y + i (Δ 2 x p x +Δ 2 y p y )-wave paired fermions on a square lattice, with tunable paring order parameters. We derive a universal phase diagram for this general p -wave theory which contains a gapped A-phase and a topologically non-trivial B-phase. We show that the gapless condition in the B-phase is governed by a generalized inversion (G-inversion) symmetry under p x ↔ (Δ 1 y / Δ 1 x ) p y . The G-inversion symmetric gapless B-phase near the phase boundaries is described by (1+1)-dimensional gapless Majorana fermions in the asymptotic long-wavelength limit, i.e. the c =1/2 conformal field theory. The gapped B-phase has G-inversion symmetry breaking and is the weak pairing phase described by the Moore-Read Pfaffian. We show that in the gapped B-phase, vortex pair excitations are separated from the ground state by a finite energy gap.