Abstract

In a bipartite set-up, the vacuum state of a free Bosonic scalar field is entangled in real space and satisfies the area-law— entanglement entropy scales linearly with area of the boundary between the two partitions. In this work, we show that the area law is violated in two spatial dimensional model Hamiltonian having dynamical critical exponent z = 3. The model physically corresponds to next-to-next-to-next nearest neighbour coupling terms on a lattice. The result reported here is the first of its kind of violation of area law in Bosonic systems in higher dimensions and signals the evidence of a quantum phase transition. We provide evidence for quantum phase transition both numerically and analytically using quantum Information tools like entanglement spectra, quantum fidelity, and gap in the energy spectra. We identify the cause for this transition due to the accumulation of large number of angular zero modes around the critical point which catalyses the change in the ground state wave function due to the next-to-next-to-next nearest neighbor coupling. Lastly, using Hubbard-Stratanovich transformation, we show that the effective Bosonic Hamiltonian can be obtained from an interacting fermionic theory and provide possible implications for condensed matter systems.

Highlights

  • Quantum field theory plays a crucial role in understanding some of the interesting features of low-temperature condensed matter systems[1,2]

  • We study the effect of next-to-next-to- nearest neighbor (NNN) coupling terms on the quantum fluctuations

  • In two dimensions, next nearest neighbor (NNN) coupling introduces instability and drive quantum fluctuations leading to quantum phase transitions (QPTs)

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Summary

Model and Setup

We discuss the model Hamiltonian and provide essential steps to obtain entanglement entropy. We show how our model Hamiltonian can be mapped to a system of coupled harmonic oscillators. Before going to the details, we briefly discuss some of the salient features of the model Hamiltonian in Eq (1): (i) The above Hamiltonian corresponds to free field with a non-linear dispersion relation between frequency ω and wave number k via, ω2 = k2 + ε k4/κ2 + τ k6/κ4. In the quantum Lifshitz transition, scalar field theory has dynamical critical exponent z = 2 and the dispersion relation is ω2 = k2 + ε k4/κ22,12,23. To map the model Hamiltonian (1) to a system of coupled harmonic oscillators; we perform integration over the angular coordinate θ by invoking orthogonal properties of cosine functions. −Tr (ρred logρred)[39,48]

DetΛ πN
Results
Ground state energy eigenvalue for case II π
Tr GΞ
Additional Information
Full Text
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