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$\mathbb{Z}_2$ Pfaffian Invariant and Entanglement Spectrum Signatures in Disordered Majorana Wires

Rowan Brad Quni-Gudzinas

Published Sep 7, 2026• 0 citations
Publisher

Abstract

In a one-dimensional (1D) disordered superconducting wire (Kitaev chain), the topological phase hosts Majorana zero modes (MZMs) at its boundaries, while the trivial phase hosts ordinary fermionic states. We identify the $\mathbb{Z}_2$ Pfaffian invariant, defined as the sign of the Pfaffian of the real-space Majorana Hamiltonian matrix, as the precise topological invariant distinguishing these phases in the presence of strong disorder. We demonstrate that this invariant is exactly mirrored in the ground-state entanglement spectrum (ES). By bipartitioning the chain, the reduced density matrix of the ground state can be expressed via an entanglement Hamiltonian determined by the restricted single-particle correlation matrix. The $\mathbb{Z}_2$ invariant is computed as the sign of the Pfaffian of the restricted correlation matrix, tracking the parity of its negative eigenvalues. In the trivial phase, the ES is non-degenerate; in the topological phase, the ES exhibits a universal two-fold degeneracy. The sign flip of this Pfaffian provides a sharp, falsifiable signature of the topological phase transition, robust to local disorder. ## 1. Introduction The Kitaev chain, a one-dimensional (1D) p-wave superconducting wire, provides a paradigmatic model for topological superconductivity. In its topological phase, the wire hosts Majorana zero modes (MZMs)—operators that are their own antiparticles—at its boundaries. In the presence of strong disorder, the distinction between the topological phase and the trivial phase hosting ordinary fermionic states becomes subtle, as momentum-space topological invariants are ill-defined. This raises the question of what precise topological invariant distinguishes these phases in real space, and whether this invariant can be extracted from the ground-state entanglement spectrum (ES) to provide a falsifiable, non-local signature of the topological phase transition. Here, we show that the $\mathbb{Z}_2$ Pfaffian invariant of the real-space M

DOI
10.5281/zenodo.22626417

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Z2\mathbb{Z}_2Z2​ Pfaffian Invariant and Entanglement Spectrum Signatures in Disordered Majorana Wires
In a one-dimensional (1D) disordered superconducting wire (Kitaev chain), the topological phase hosts Majorana zero modes (MZMs) at its boundaries, while the trivial phase hosts ordinary fermionic states. We identify the Z2\mathbb{Z}_2Z2​ Pfaffian invariant, defined as the sign of the Pfaffian of the real-space Majorana Hamiltonian matrix, as the precise topological invariant distinguishing these phases in the presence of strong disorder. We demonstrate that this invariant is exactly mirrored in the ground-state entanglement spectrum (ES). By bipartitioning the chain, the reduced density matrix of the ground state can be expressed via an entanglement Hamiltonian determined by the restricted single-particle correlation matrix. The Z2\mathbb{Z}_2Z2​ invariant is computed as the sign of the Pfaffian of the restricted correlation matrix, tracking the parity of its negative eigenvalues. In the trivial phase, the ES is non-degenerate; in the topological phase, the ES exhibits a universal two-fold degeneracy. The sign flip of this Pfaffian provides a sharp, falsifiable signature of the topological phase transition, robust to local disorder. ## 1. Introduction The Kitaev chain, a one-dimensional (1D) p-wave superconducting wire, provides a paradigmatic model for topological superconductivity. In its topological phase, the wire hosts Majorana zero modes (MZMs)—operators that are their own antiparticles—at its boundaries. In the presence of strong disorder, the distinction between the topological phase and the trivial phase hosting ordinary fermionic states becomes subtle, as momentum-space topological invariants are ill-defined. This raises the question of what precise topological invariant distinguishes these phases in real space, and whether this invariant can be extracted from the ground-state entanglement spectrum (ES) to provide a falsifiable, non-local signature of the topological phase transition. Here, we show that the Z2\mathbb{Z}_2Z2​ Pfaffian invariant of the real-space M
Topological superconductors in one spatial dimension exhibiting a single Majorana bound state at each end are distinguished from trivial gapped systems by a Z2{\mathbb{Z}}_{2}Z2​ topological invariant. Originally, this invariant was calculated by Kitaev in terms of the Pfaffian of the Majorana representation of the Hamiltonian: The sign of this Pfaffian divides the set of all gapped quadratic forms of Majorana fermions into two inequivalent classes. In the more familiar Bogoliubov de Gennes mean-field description of superconductivity, an emergent particle-hole symmetry gives rise to a quantized Zak-Berry phase, the value of which is also a topological invariant. In this work, we explicitly show the equivalence of these two formulations by relating both of them to the phase winding of the transformation matrix that brings the Majorana representation matrix of the Hamiltonian into its Jordan normal form.
We investigate the topological phases of two one-dimensional (1D) interacting superconducting wires and propose topological markers directly measurable from ground-state correlation functions. These quantities remain powerful tools in the presence of couplings and interactions. We show with the density matrix renormalization group that the double critical Ising (DCI) phase of two interacting Kitaev chains is a fractional topological phase with gapless Majorana modes in the bulk, and a one-half topological invariant per wire. Using both numerics and quantum field theoretical methods, we show that the phase diagram remains stable in the presence of an interwire hopping amplitude ${t}_{\ensuremath{\perp}}$ at length scales below $\ensuremath{\sim}1/{t}_{\ensuremath{\perp}}$. A large interwire hopping amplitude results in the emergence of two integer topological phases, stable also at large interactions. They host one edge mode per boundary shared between both wires. At large interactions, the two wires are described by Mott physics, with the ${t}_{\ensuremath{\perp}}$ hopping amplitude resulting in a paramagnetic order.
We investigate the spectral and topological properties of a zigzag Kitaev chain constructed from two diagonally coupled one dimensional Kitaev chains with a zero and finite superconducting pairing phase difference. Using a Bogoliubov-de Gennes formulation, we analyze the energy spectrum, distribution of Majorana zero modes (MZMs), the quasi-particle dispersion, and the winding number, respectively. For a zero phase difference, the resulting energy spectrum shows topological phases with two, four MZMs, and trivial regions. The phases of gap closure determine the topological phase boundaries. In particular, for the phase difference between φ=πφ=πφ=π, the degeneracy of MZMs is partially lifted, leading to modified topological phases compared to the case φ=0φ=0φ=0. The topological and trivial phase boundaries are further confirmed by evaluating the quasi-particle dispersion and the topological invariant, namely the winding number. We show that the zigzag Kitaev chain contributes independently to the total winding number ν=1ν= 1ν=1 and 222, giving rise to distinct topological phases that support two and four MZMs. The ν=0ν= 0ν=0 gives rise to a trivial region. The energy spectrum of systems corroborates the analytical phase boundaries and reveals characteristics associated with hybridization, enabling us to obtain the complete phase diagram of the zigzag model. Our results establish the zigzag Kitaev chain as a minimal platform for engineering MZM quantum computations, with potential applications in the study of topological phases and Majorana based qubit physics.
This thesis is devoted to the topic of one- and two-dimensional models of topological superconductivity. We study the Kitaev chain subject to closed and open boundary conditions. In the closed chain, we derive the energy spectrum, the ground state, and the topological invariant viewed as a certain Berry phase. We study two-point correlation functions and find enlarged values close to the topological phase transitions. The open chain is studied with focus on describing the degenerate ground states for a simple parameter choice in the topological phase. Then, the open system Hamiltonian is diagonalized numerically, and we model the order parameter with a spatial dependency. Additional Majorana zero modes appear if the order parameter changes sign. We also consider the p+ip model. The localization of a Majorana zero mode, bound to a vortex that is described by Ginzburg-Landau theory, is found numerically. We propose an argument that results in a non-Abelian exchange transformation for a system of several vortices. The p+ip model is also studied on an annulus; we approximate the ground state as a combination of boundary states and calculate its energy. The results are compared to a numerical implementation, and the agreement is convincing as the boundary separation becomes large compared to other length scales.
We study the decay and oscillations of Majorana fermion wave functions and ground-state (GS) fermion parity in one-dimensional topological superconducting lattice systems. Using a Majorana transfer matrix method, we find that Majorana wave-function properties are encoded in the associated Lyapunov exponent, which in turn is the sum of two independent components: a ``superconducting component,'' which characterizes the gap induced decay, and the ``normal component,'' which determines the oscillations and response to chemical potential configurations. The topological phase transition separating phases with and without Majorana end modes is seen to be a cancellation of these two components. We show that Majorana wave-function oscillations are completely determined by an underlying nonsuperconducting tight-binding model and are solely responsible for GS fermion parity switches in finite-sized systems. These observations enable us to analytically chart out wave-function oscillations, the resultant GS parity configuration as a function of parameter space in uniform wires, and special parity switch points where degenerate zero energy Majorana modes are restored in spite of finite size effects. For disordered wires, we find that band oscillations are completely washed out leading to a second localization length for the Majorana mode and the remnant oscillations are randomized as per Anderson localization physics in normal systems. Our transfer matrix method further allows us to (i) reproduce known results on the scaling of midgap Majorana states and demonstrate the origin of its log-normal distribution, (ii) identify contrasting behavior of disorder-dependent GS parity switches for the cases of even versus odd number of lattice sites, and (iii) chart out the GS parity configuration and associated parity switch points as a function of disorder strength.
Abstract Semiconducting nanowires with strong Rashba spin–orbit coupling in the proximity with a superconductor and under a strong Zeeman field can potentially manifest Majorana zero modes (MZMs) at their edges and are a topical candidate for topological superconductivity. However, protocols for their detection based on the local and the non-local conductance spectroscopy have been subject to intense scrutiny. In this work, by taking current experimental setups into account, we detail mathematical ideas related to the entanglement entropy and the fermion parity fluctuations to faithfully distinguish between true MZMs and trivial quasi-MZMs. We demonstrate that the disconnected entanglement entropy, derived from the von Neumann entanglement entropy, provides a distinct and robust signature of the topological phase transition which is immune to system parameters, size and disorders. In order to understand the entanglement entropy of the Rashba nanowire system, we establish its connection to a model of interacting spinfull Kitaev chains. Moreover, we relate the entanglement entropy to the fermionic parity fluctuation, and show that it behaves concordantly with entanglement entropy, hence making it a suitable metric for the detection of MZMs. In connection with the topological gap protocol that is based on the conductance spectra, the aforesaid metrics can reliably point toward the topological transitions even in realistic setups.