Professional Education
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PhD, University of California, Santa Barbara (2022)
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BSc, Fudan University (2016)
All Publications
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Phase diagram of the three-dimensional subsystem toric code
PHYSICAL REVIEW RESEARCH
2024; 6 (4)
View details for DOI 10.1103/PhysRevResearch.6.043007
View details for Web of Science ID 001329816500003
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Continuous symmetry breaking in adaptive quantum dynamics
PHYSICAL REVIEW B
2024; 109 (21)
View details for DOI 10.1103/PhysRevB.109.214305
View details for Web of Science ID 001248729200003
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Statistical mechanics model for Clifford random tensor networks and monitored quantum circuits
PHYSICAL REVIEW B
2024; 109 (17)
View details for DOI 10.1103/PhysRevB.109.174307
View details for Web of Science ID 001236724100001
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Decodable hybrid dynamics of open quantum systems with Z2 symmetry
PHYSICAL REVIEW B
2023; 108 (21)
View details for DOI 10.1103/PhysRevB.108.214302
View details for Web of Science ID 001141798900002
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Operator Relaxation and the Optimal Depth of Classical Shadows.
Physical review letters
2023; 130 (23): 230403
Abstract
Classical shadows are a powerful method for learning many properties of quantum states in a sample-efficient manner, by making use of randomized measurements. Here we study the sample complexity of learning the expectation value of Pauli operators via "shallow shadows," a recently proposed version of classical shadows in which the randomization step is effected by a local unitary circuit of variable depth t. We show that the shadow norm (the quantity controlling the sample complexity) is expressed in terms of properties of the Heisenberg time evolution of operators under the randomizing ("twirling") circuit-namely the evolution of the weight distribution characterizing the number of sites on which an operator acts nontrivially. For spatially contiguous Pauli operators of weight k, this entails a competition between two processes: operator spreading (whereby the support of an operator grows over time, increasing its weight) and operator relaxation (whereby the bulk of the operator develops an equilibrium density of identity operators, decreasing its weight). From this simple picture we derive (i) an upper bound on the shadow norm which, for depth t∼log(k), guarantees an exponential gain in sample complexity over the t=0 protocol in any spatial dimension, and (ii) quantitative results in one dimension within a mean-field approximation, including a universal subleading correction to the optimal depth, found to be in excellent agreement with infinite matrix product state numerical simulations. Our Letter connects fundamental ideas in quantum many-body dynamics to applications in quantum information science, and paves the way to highly optimized protocols for learning different properties of quantum states.
View details for DOI 10.1103/PhysRevLett.130.230403
View details for PubMedID 37354418
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Triviality of quantum trajectories close to a directed percolation transition
PHYSICAL REVIEW B
2023; 107 (22)
View details for DOI 10.1103/PhysRevB.107.224303
View details for Web of Science ID 001016217000002
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Cross Entropy Benchmark for Measurement-Induced Phase Transitions.
Physical review letters
2023; 130 (22): 220404
Abstract
We investigate prospects of employing the linear cross entropy to experimentally access measurement-induced phase transitions without requiring any postselection of quantum trajectories. For two random circuits that are identical in the bulk but with different initial states, the linear cross entropy χ between the bulk measurement outcome distributions in the two circuits acts as an order parameter, and can be used to distinguish the volume law from area law phases. In the volume law phase (and in the thermodynamic limit) the bulk measurements cannot distinguish between the two different initial states, and χ=1. In the area law phase χ<1. For circuits with Clifford gates, we provide numerical evidence that χ can be sampled to accuracy ϵ from O(1/ϵ^{2}) trajectories, by running the first circuit on a quantum simulator without postselection, aided by a classical simulation of the second. We also find that for weak depolarizing noise the signature of the measurement-induced phase transitions is still present for intermediate system sizes. In our protocol we have the freedom of choosing initial states such that the "classical" side can be simulated efficiently, while simulating the "quantum" side is still classically hard.
View details for DOI 10.1103/PhysRevLett.130.220404
View details for PubMedID 37327428
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Entanglement Domain Walls in Monitored Quantum Circuits and the Directed Polymer in a Random Environment
PRX QUANTUM
2022; 4 (1)
View details for DOI 10.1103/PRXQuantum.4.010331
View details for Web of Science ID 000972726000001
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Entanglement phase transitions in random stabilizer tensor networks
PHYSICAL REVIEW B
2022; 105 (10)
View details for DOI 10.1103/PhysRevB.105.104306
View details for Web of Science ID 000771393800004
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Conformal invariance and quantum nonlocality in critical hybrid circuits
PHYSICAL REVIEW B
2021; 104 (10)
View details for DOI 10.1103/PhysRevB.104.104305
View details for Web of Science ID 000696023400002
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Entanglement Negativity at Measurement-Induced Criticality
PRX QUANTUM
2021; 2 (3)
View details for DOI 10.1103/PRXQuantum.2.030313
View details for Web of Science ID 000680527000001
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Statistical mechanics of quantum error correcting codes
PHYSICAL REVIEW B
2021; 103 (10)
View details for DOI 10.1103/PhysRevB.103.104306
View details for Web of Science ID 000646626700003
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Emergent conformal symmetry in nonunitary random dynamics of free fermions
PHYSICAL REVIEW RESEARCH
2020; 2 (3)
View details for DOI 10.1103/PhysRevResearch.2.033017
View details for Web of Science ID 000604137500002
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Measurement-driven entanglement transition in hybrid quantum circuits
PHYSICAL REVIEW B
2019; 100 (13)
View details for DOI 10.1103/PhysRevB.100.134306
View details for Web of Science ID 000490166700003
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Quantum Zeno effect and the many-body entanglement transition
PHYSICAL REVIEW B
2018; 98 (20)
View details for DOI 10.1103/PhysRevB.98.205136
View details for Web of Science ID 000450548500005