Sivaprasad Omanakuttan

Regularized Warm-Started Quantum Approximate Optimization and Conditions for Surpassing Classical Solvers on the Max-Cut Problem

Zichang He, Anuj Apte, Brandon Augustino, Arman Babakhani, Abid Khan [1], Sivaprasad Omanakuttan [1], Ruslan Shaydulin [1]

Abstract

Demonstrating quantum heuristics that outperform strong classical solvers on large-scale optimization remains an open challenge. Here we introduce Regularized Warm-Started QAOA (RWS-QAOA), which initializes qubits by minimizing expected energy with a regularizer that penalizes near-bitstring states, preventing QAOA from stalling. We further propose a protocol that yields fixed, instance-independent parameters, enabling RWS-QAOA to operate as a non-variational algorithm in which the quantum circuit parameters are fixed and only a classical warm starting step is instance-dependent. We evaluate RWS-QAOA on the Max-Cut problem for random regular graphs, where this protocol yields a constant-depth quantum circuit, across three complementary settings. First, on Quantinuum's trapped-ion processor, RWS-QAOA outperforms the classical algorithms with the best provable guarantees for Max-Cut on $3$-regular graphs, namely Goemans-Williamson and Halperin-Livnat-Zwick, on $96$-node instances. Second, tensor-network simulations on graphs with up to $N{=}10{,}000$ nodes show that depth-$6$ RWS-QAOA, achieving an average cut fraction of $0.9167$, surpasses the best classical heuristics under matched restrictions (no local-search post-processing and no iterative refinement). Third, we remove these restrictions and benchmark against the strongest unrestricted classical heuristics, including an optimized parallel Burer-Monteiro solver that improves upon the MQLib implementation. Even against this stronger baseline, we project that surface-code RWS-QAOA reaches a quantum-classical runtime crossover below $0.2$ seconds on $3{,}000$-node graphs with fewer than $1.3$ million physical qubits. Our results show that constant-depth quantum circuits combined with a classical warm start have a credible potential to surpass classical solvers on the Max-Cut problem when executed on future quantum computers.

Certified randomness amplification by dynamically probing remote random quantum states

Minzhao Liu [1], Pradeep Niroula [1], Matthew DeCross [2], Cameron Foreman [3], Wen Yu Kon [1], Ignatius William Primaatmaja [1,2], M. S. Allman, J. P. Campora, Akhil Isanaka [2], Kartik Singhal [2], Omar Amer [1], Shouvanik Chakrabarti [1], Kaushik Chakraborty [1], Samuel F. Cooper [2], Robert D. Delaney [2], Joan M. Dreiling [2], Brian Estey [2], Caroline Figgatt [2], Cameron Foltz [2], John P. Gaebler [2], Alex Hall [2], Zichang He [1], Craig A. Holliman [4], Travis S. Humble [5], Shih-Han Hung [6], Ali A. Husain [7], Yuwei Jin [1], Fatih Kaleoglu [1], Colin J. Kennedy [2], Nikhil Kotibhaskar [3], Nathan K. Lysne [4], Ivaylo S. Madjarov [2], Michael Mills [2], Alistair R. Milne [3], Kevin Milner [3], Louis Narmour [2], Sivaprasad Omanakuttan [1], Annie J. Park [2], Michael A. Perlin [1], Adam P. Reed [2], Chris N. Self [8], Matthew Steinberg [1], David T. Stephen [2], Joseph Sullivan [1], Alex Chernoguzov [2], Florian J. Curchod [8], Anthony Ransford [2], Justin G. Bohnet [2], Brian Neyenhuis [2], Michael Foss-Feig [2], Rob Otter [1], Ruslan Shaydulin [1]

Abstract

Cryptography depends on truly unpredictable numbers, but physical sources emit biased or correlated bits. Quantum mechanics enables the amplification of imperfect randomness into nearly perfect randomness, but prior demonstrations have required physically co-located, loophole-free Bell tests, constraining the feasibility of remote operation. Here we realize certified randomness amplification across a network by dynamically probing large, entangled quantum states on Quantinuum's 98-qubit Helios trapped-ion quantum processor. Our protocol is secure even if the remote device acts maliciously or is compromised by an intercepting adversary, provided the samples are generated quickly enough to preclude classical simulation of the quantum circuits. We stream quantum gates in real time to the quantum processor, maintain quantum state coherence for $\approx 0.9$ seconds, and then reveal the measurement bases to the quantum processor only milliseconds before measurement. This limits the time for classical spoofing to 30 ms and constrains the location of hypothetical adversaries to a $4{,}500$ km radius. We achieve a fidelity of 0.586 on random circuits with 64 qubits and 276 two-qubit gates, enabling the amplification of realistic imperfect randomness with a low entropy rate into nearly perfect randomness.

Realization of a Quantum Streaming Algorithm on Long-lived Trapped-ion Qubits

Pradeep Niroula [1], Shouvanik Chakrabarti [1], Steven Kordonowy [1], Niraj Kumar [1], Sivaprasad Omanakuttan [1], Michael A. Perlin [1,2], M. S. Allman, J. P. Campora, Alex Chernoguzov [2], Samuel F. Cooper [2], Robert D. Delaney [2], Joan M. Dreiling [2], Brian Estey [2], Caroline Figgatt [2], Cameron Foltz [2], John P. Gaebler [2], Alex Hall [2], Ali A. Husain [3], Akhil Isanaka [2], Colin J. Kennedy [2], Nikhil Kotibhaskar [4], Ivaylo S. Madjarov [2], Michael Mills [2], Alistair R. Milne [4], Louis Narmour [2], Annie J. Park [2], Adam P. Reed [2], Kartik Singhal [2], Anthony Ransford [2], Justin G. Bohnet [2], Brian Neyenhuis [2], Rob Otter [1], Ruslan Shaydulin [1]

Abstract

Large classical datasets are often processed in the streaming model, with data arriving one item at a time. In this model, quantum algorithms have been shown to offer an unconditional exponential advantage in space. However, experimentally implementing such streaming algorithms requires qubits that remain coherent while interacting with an external data stream. In this work, we realize such a data-streaming model using Quantinuum Helios trapped-ion quantum computer with long-lived qubits that communicate with an external server. We implement a quantum pair sketch, which is the primitive underlying many quantum streaming algorithms, and use it to solve Hidden Matching, a problem known to exhibit a theoretical exponential quantum advantage in space. Furthermore, we compile the quantum streaming algorithm to fault-tolerant quantum architectures based on surface and bivariate bicycle codes and show that the quantum space advantage persists even with the overheads of fault-tolerance.

Iceberg Beyond the Tip: Co-Compilation of a Quantum Error Detection Code and a Quantum Algorithm

Yuwei Jin, Zichang He, Tianyi Hao, Sivaprasad Omanakuttan, David Amaro, Swamit Tannu, Ruslan Shaydulin, Marco Pistoia [1]

Abstract

The rapid progress in quantum hardware is expected to make them viable tools for the study of quantum algorithms in the near term. The timeline to useful algorithmic experimentation can be accelerated by techniques that use many noisy shots to produce an accurate estimate of the observable of interest. One such technique is to encode the quantum circuit using an error detection code and discard the samples for which an error has been detected. An underexplored property of error-detecting codes is the flexibility in the circuit encoding and fault-tolerant gadgets, which enables their co-optimization with the algorthmic circuit. However, standard circuit optimization tools cannot be used to exploit this flexibility as optimization must preserve the fault-tolerance of the gadget. In this work, we focus on the $[[k+2, k, 2]]$ Iceberg quantum error detection code, which is tailored to trapped-ion quantum processors. We design new flexible fault-tolerant gadgets for the Iceberg code, which we then co-optimize with the algorithmic circuit for the quantum approximate optimization algorithm (QAOA) using tree search. By co-optimizing the QAOA circuit and the Iceberg gadgets, we achieve an improvement in QAOA success probability from $44\%$ to $65\%$ and an increase in post-selection rate from $4\%$ to $33\%$ at 22 algorithmic qubits, utilizing 330 algorithmic two-qubit gates and 744 physical two-qubit gates on the Quantinuum H2-1 quantum computer, compared to the previous state-of-the-art hardware demonstration. Furthermore, we demonstrate better-than-unencoded performance for up to 34 algorithmic qubits, employing 510 algorithmic two-qubit gates and 1140 physical two-qubit gates.