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Observation of higher-order topological states on a quantum computer

Jin Ming Koh, Tommy Tai, Ching Hua Lee · 2023 · 3 citationsRead the paper

Programmable quantum simulators such as superconducting quantum processors and ultracold atomic lattices represent rapidly developing emergent technology that may one day qualitatively outperform existing classical computers. Yet, apart from a few breakthroughs, the range of viable computational applications with current-day noisy intermediate-scale quantum (NISQ) devices is still significantly limited by gate errors, quantum decoherence, and the number of high-quality qubits. In this work, we develop an approach that places NISQ hardware as a particularly suitable platform for simulating multi-dimensional condensed matter systems, including lattices beyond three dimensions which are difficult to realize or probe in other settings. By fully exploiting the exponentially large Hilbert space of a quantum chain, we encoded a high-dimensional model in terms of non-local many-body interactions that can further be systematically transcribed into quantum gates. We demonstrate the power of our approach by realizing, on IBM transmon-based quantum computers, higher-order topological states in up to four dimensions, which are exotic phases that have never been realized in any quantum setting. With the aid of in-house circuit compression and error mitigation techniques, we measured the topological state dynamics and their protected mid-gap spectra to a high degree of accuracy, as benchmarked by reference exact diagonalization data. The time and memory needed with our approach scale favorably with system size and dimensionality compared to exact diagonalization on classical computers.

What the full text shows

Working prototype
  • Realized higher-order topological (HOT) states in up to four dimensions (tesseract) on a quantum processor. — up to 4 dimensions (IBM transmon-based quantum computers)
  • Measured the correct degeneracy of midgap HOT modes for 2D square lattice configurations (C0, C2, and C4). — 0, 2, and 4 midgap zero modes (10x10 HOT lattice encoded on a 20-qubit chain plus one ancillary qubit)
  • Demonstrated topological robustness where states localized on topological corners exhibit significantly slowed decay compared to non-protected states. — occupancy fidelity remains near unity over time (16x16 HOT lattices mapped onto 32-qubit chains)
Setup
IBM transmon-based superconducting devices (ibmq_manhattan, ibmq_brooklyn, ibmq_sydney, ibmq_toronto, ibmq_mumbai, ibmq_montreal) with 27 to 65 qubits; T1/T2 times 80-130 μs; single-qubit gate errors O(10^-4) and two-qubit gate errors O(10^-2).
How
The researchers mapped d-dimensional non-interacting lattices to 1D interacting hardcore boson chains, which were then transcribed into quantum gates using first-order Trotterization. They used Iterative Quantum Phase Estimation (IQPE) to probe midgap spectra and measured site-resolved occupancy densities to assess state dynamics.
Limitations
Limited by gate errors, quantum decoherence, and the number of high-quality qubits in NISQ hardware. · Requires circuit compression and error mitigation to achieve high accuracy. · Scalable realization of larger HOT systems requires hardware exceeding present capabilities.

Summarized by Gemma 4 from the open-access full text · 12 Oct 2026. Read it