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Theoretical physicists working at a blackboard collaboration pod in the Beecroft building.
Credit: Jack Hobhouse

Dr. Natalia Chepiga

Royal Society University Research Fellow

Research theme

  • Fields, strings, and quantum dynamics
  • Quantum information and computation

Sub department

  • Rudolf Peierls Centre for Theoretical Physics
natalia.chepiga@physics.ox.ac.uk
personal website
  • About
  • Publications

Exact zero modes in interacting Majorana X- and Y-junctions

ArXiv 2506.10898 (2025)

Authors:

Bowy M La Rivière, Rik Mulder, Natalia Chepiga
Details from ArXiV

Deconfined quantum criticality in a frustrated Haldane chain with single-ion anisotropy

ArXiv 2503.11413 (2025)

Authors:

Niels T Pronk, Bowy M La Rivière, Natalia Chepiga
Details from ArXiV

Numerical investigation of quantum phases and phase transitions in a two-leg ladder of Rydberg atoms

Physical Review Research American Physical Society (APS) 7:1 (2025) 013215

Authors:

Jose Soto-Garcia, Natalia Chepiga

Abstract:

Experiments on chains of Rydberg atoms appear as a playground to study quantum phase transitions in 1D. As a natural extension, we report a quantitative ground-state phase diagram of Rydberg atoms arranged in a two-leg ladder interacting via van der Waals potential. We address this problem numerically, using the density matrix renormalization group algorithm. Our results suggest that, quite remarkably, Z k crystalline phases, with the exception of the checkerboard phase, appear in pairs characterized by the same pattern of occupied rungs but distinguishable by a spontaneously broken Z ̃ 2 symmetry between the two legs of the ladder. Within each pair, the two phases are separated by a continuous transition in the Ising universality class, which eventually fuses with the Z k transition, whose nature depends on k . According to our results, the transition into the Z 2 ⊗ Z ̃ 2 phase changes its nature multiple times, including an Ashkin-Teller transition that is surprisingly stable over an extended interval, followed by the Z 4 -chiral transition, and finally in a two step-process mediated melting via the floating phase. The transition into the Z 3 phase with resonant states on the rungs belongs to the three-state Potts universality class at the commensurate point, to the Z 3 -chiral Huse-Fisher universality class away from it, and eventually it is through an intermediate floating phase. The Ising transition between Z 3 and Z 3 ⊗ Z ̃ 2 phases, entering the floating phase, opens the possibility to realize lattice supersymmetry in Rydberg quantum simulators.
More details from the publisher
More details

The quantum Kibble-Zurek mechanism: the role of boundary conditions, endpoints and kink types

ArXiv 2412.20186 (2024)

Authors:

Jose Soto Garcia, Natalia Chepiga
Details from ArXiV

A tensor network formulation of Lattice Gauge Theories based only on symmetric tensors

ArXiv 2412.16961 (2024)

Authors:

Manu Canals, Natalia Chepiga, Luca Tagliacozzo
Details from ArXiV

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