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

Siddharth Parameswaran

Professor of Physics

Research theme

  • Fields, strings, and quantum dynamics
  • Quantum materials
  • Quantum optics & ultra-cold matter

Sub department

  • Rudolf Peierls Centre for Theoretical Physics

Research groups

  • Condensed Matter Theory
sid.parameswaran@physics.ox.ac.uk
Telephone: 01865 273968
Rudolf Peierls Centre for Theoretical Physics, room 70.29
Hilary Term 2026: Quantum Matter 2 Course Pages
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Efficient quantum thermal state preparation via local driving: Lindbladian simulation with provable guarantees

Physical Review B American Physical Society (APS) 114:1 (2026) 14302

Authors:

Dominik Hahn, Sa Parameswaran, Benedikt Placke

Abstract:

<jats:p> Preparing the thermal density matrix <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"> <a:mrow> <a:msub> <a:mi>ρ</a:mi> <a:mi>β</a:mi> </a:msub> <a:mo>∝</a:mo> <a:msup> <a:mi>e</a:mi> <a:mrow> <a:mo>−</a:mo> <a:mi>β</a:mi> <a:mi>H</a:mi> </a:mrow> </a:msup> </a:mrow> </a:math> corresponding to a given Hamiltonian <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"> <b:mi>H</b:mi> </b:math> is a task of central interest across quantum many-body physics, and is particularly salient when attempting to study it with quantum computers. Although solved in principle by recent constructions of efficiently simulable Lindblad master equations—that provably have <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"> <c:msub> <c:mi>ρ</c:mi> <c:mi>β</c:mi> </c:msub> </c:math> as a steady state [C.-F. Chen , ]—the implementation of these “exact Gibbs samplers” requires large-scale quantum computing resources and is hence challenging in practice on current or even near-term quantum devices. Here, we propose a scheme for approximately simulating an exact Gibbs sampler up to a rigorously bounded error that only requires the (repeated) implementation of three readily available ingredients: (a) analog simulation of <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"> <d:mi>H</d:mi> </d:math> ; (b) strictly local but time-dependent couplings to ancilla qubits; and (c) reset of the ancillas. We give rigorous guarantees on the difference between the fixed point reached by our protocol and the exact thermal state, which only depend on parameters of the protocol and its . The procedure is efficiently implementable on near-term devices if <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"> <e:mi>H</e:mi> </e:math> is local and the mixing time scales mildly with both system size and protocol parameters. While guaranteeing the latter for Hamiltonians of interest remains an important problem for future work, here we lay the groundwork for developing fully efficient thermal state preparation protocols on quantum simulators. </jats:p>
More details from the publisher

Engineering electrically-switchable quantum anomalous Hall states by spin-orbit coupling

(2026)

Authors:

Maosen Qin, Ziwei Wang, Gyeongmin Kim, Kenji Watanabe, Takashi Taniguchi, Steven H Simon, Siddharth A Parameswaran, Hryhoriy Polshyn
More details from the publisher

Hidden antiferromagnetism, persistent valley fluctuations, and $U(6)$ crossovers in triangular-lattice M-point moiré materials via determinantal quantum Monte Carlo

(2026)

Authors:

Konstantinos Vasiliou, Dumitru Călugăru, Johannes S Hofmann, SA Parameswaran
More details from the publisher

Mixed-dimensional quantum Monte Carlo studies of M-point moiré materials

(2026)

Authors:

Dumitru Călugăru, Konstantinos Vasiliou, Haoyu Hu, B Andrei Bernevig, Werner Krauth, SA Parameswaran
More details from the publisher

Rigorous error bounds for dissipative thermal state preparation from weak system-bath coupling

(2026)

Authors:

Christopher Ong, SA Parameswaran, Benedikt Placke, Dominik Hahn
More details from the publisher

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