2022
DOI: 10.1103/physrevlett.129.140502
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Simulation of Interaction-Induced Chiral Topological Dynamics on a Digital Quantum Computer

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Cited by 18 publications
(13 citation statements)
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“…where u α π is now labeled by the parity vector π of lattice coordinates, and the parity operator Recompilation. Circuit recompilation starts from a circuit ansatz, whose parameters are dynamically optimized [76][77][78][79][80]134]. We use a circuit ansatz comprising an initial layer of U3 general single-qubit rotation gates on all qubits followed by K ansatz layers, each comprising a layer of CX gates entangling adjacent qubits and a layer of U3 rotations (see Figure 2e).…”
Section: Methodsmentioning
confidence: 99%
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“…where u α π is now labeled by the parity vector π of lattice coordinates, and the parity operator Recompilation. Circuit recompilation starts from a circuit ansatz, whose parameters are dynamically optimized [76][77][78][79][80]134]. We use a circuit ansatz comprising an initial layer of U3 general single-qubit rotation gates on all qubits followed by K ansatz layers, each comprising a layer of CX gates entangling adjacent qubits and a layer of U3 rotations (see Figure 2e).…”
Section: Methodsmentioning
confidence: 99%
“…However, while straightforward, such an approach yields deep circuits unsuitable for presentgeneration NISQ hardware. To compress the circuits, we utilize a tensor network-aided recompilation technique [76][77][78][79][80]. We exploit the number-conserving symmetries of H dD chain , arising from H dD lattice and the nature of our mapping (see Methods), to enhance circuit construction performance and quality at large circuit breadths (up to 32 qubits).…”
Section: B Simulation On Quantum Hardwarementioning
confidence: 99%
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“…The rapid development of hardware and algorithms in universal quantum computation also opens up the possibility of implementing our YLES measurement protocol in quantum computers via ancilla-based methods [88][89][90][91]. Moreover, our MPS implementation, which is related to mid-circuit measurements [92][93][94][95], provides an approach to improve the current ancilla-based methods for dynamically simulating various non-Hermitian many-body phenomena [96][97][98][99][100][101][102][103] and unconventional non-Hermitian topology [104][105][106][107][108][109][110][111][112][113][114][115][116][117], on quantum circuits.…”
Section: (B) Upon Obtaining γ ∞mentioning
confidence: 99%
“…As discussed in Appendix A, although a uniform grounding mechanism can be employed to isolate the topological states isolated from the bulk states, a Chern topolectrical circuit can be designed so that it exhibits clear chiral propagating boundary states in the admittance spectrum without a uniform grounding mechanism. This is due to nontrivial center-of-mass pumping through a Laughlin-style pumping argument [119][120][121][122][123][124], which has been demonstrated in a variety of classical and quantum settings [18,[125][126][127][128][129]. Here, due to the nearest neighbor connections and the onsite capacitors represented by the factor σ z in the Laplacian, the topological states are separated despite the nonuniform grounding.…”
Section: Example: 2d Chern Kink Topolectrical Circuitmentioning
confidence: 99%