Trent Jacobs

Experimental validation of a compact fault-tolerant architecture for trapped ions

Noah Berthusen, Ali Lavasani, Asmae Benhemou, M. S. Allman, Joan Dreiling, Brian Estey, Cameron Foltz, Trent Jacobs, Michael Mills, Annie Jihyun Park, Adam P. Reed, David Hayes, Tzvetan S. Metodi, Andrew C. Potter

Abstract

Quantum error correction (QEC) is beginning to enable logical operations that outperform their unencoded physical counterparts, but useful fault-tolerant computation will require more than low-error quantum memory. An effective architecture must orchestrate efficient logical encoding, low-overhead logical operations, and access to the non-Clifford resources required for universal computation. Here, we introduce and experimentally validate such an architecture based on the $[[20,2,6]]$ $C_4$-Helix code, designed for the early fault-tolerant regime. Using Quantinuum Helios, a 98-qubit trapped-ion quantum processor, we experimentally demonstrate the principal components of this architecture: we perform repeated quantum error correction with an error of $4.6^{+6.2}_{-2.6}\times10^{-5}$ per logical qubit per QEC cycle. We benchmark the complete Clifford group on the two logical qubits of a single codeblock under active error correction, obtaining an error of $2.8^{+1.0}_{-1.6}\times 10^{-4}$ per two-qubit logical Clifford. We further demonstrate a fault-tolerant chain-map interface between $C_4$-Helix and a distance-5 surface code, preparing a heterogeneous three-logical-qubit GHZ state with a fidelity lower bound of $99.925^{+0.068}_{-0.245}\%$. In each case, the encoded implementation outperforms its corresponding unencoded physical baseline without relying on postselection. Circuit-level simulations indicate that improvements in physical fidelity bring the same architecture into the $10^{-6}$-$10^{-8}$ logical-error regime targeted for early fault-tolerant computation. Together, these results establish $C_4$-Helix as a hardware-validated fault-tolerant architecture rather than a bare quantum memory.

Helios: A 98-qubit trapped-ion quantum computer

Anthony Ransford [1], M. S. Allman, Jake Arkinstall [2,1], J. P. Campora, Samuel F. Cooper [1], Robert D. Delaney [1], Joan M. Dreiling [1], Brian Estey [1], Caroline Figgatt [1], Alex Hall [1], Ali A. Husain [3], Akhil Isanaka [1], Colin J. Kennedy [1], Nikhil Kotibhaskar [4], Ivaylo S. Madjarov [1], Karl Mayer [1], Alistair R. Milne [4], Annie J. Park [1], Adam P. Reed [1], Riley Ancona [1], Molly P. Andersen [5], Pablo Andres-Martinez [2], Will Angenent [2], Liz Argueta [1], Benjamin Arkin [1], Leonardo Ascarrunz [1], William Baker [1], Corey Barnes [1], John Bartolotta [1], Jordan Berg [1], Ryan Besand [1], Bryce Bjork [1], Matt Blain [5], Paul Blanchard [1], Robin Blume-Kohout [6], Matt Bohn [1,2], Agustin Borgna, Daniel Y. Botamanenko [1], Robert Boutelle [1], Natalie Brown [1], Grant T. Buckingham [1], Nathaniel Q. Burdick [3], William Cody Burton [1], Varis Carey [1], Christopher J. Carron [5], Joe Chambers [1], John Children [2], Victor E. Colussi [1], Steven Crepinsek [1], Andrew Cureton [1], Joe Davies [5], Daniel Davis [1], Matthew DeCross [1], David Deen [3], Conor Delaney [1], Davide DelVento [1], B. J. DeSalvo, Jason Dominy [1], Ross Duncan [7], Vanya Eccles [2], Alec Edgington [2], Neal Erickson [1], Stephen Erickson [1], Christopher T. Ertsgaard [5], Bruce Evans [1], Tyler Evans [1], Maya I. Fabrikant [1], Andrew Fischer [1], Cameron Foltz [1], Michael Foss-Feig [1], David Francois [1], Brad Freyberg [1], Charles Gao [1], Robert Garay [1], Jane Garvin [1], David M. Gaudiosi [1], Christopher N. Gilbreth [1], Josh Giles [1], Erin Glynn [1], Jeff Graves [1], Azure Hansen [1], David Hayes [1], Lukas Heidemann [2], Bob Higashi [5], Tyler Hilbun [1], Jordan Hines [6], Ariana Hlavaty [2], Kyle Hoffman [1], Ian M. Hoffman [1], Craig Holliman [7], Isobel Hooper [2], Bob Horning [5], James Hostetter [3], Daniel Hothem [8], Jack Houlton [1], Jared Hout [1], Ross Hutson [1], Ryan T. Jacobs [1], Trent Jacobs [1], Melf Johannsen [2], Jacob Johansen [1], Loren Jones [1], Sydney Julian [1], Ryan Jung [5], Aidan Keay [2], Todd Klein [5], Mark Koch [2], Ryo Kondo [1], Chang Kong [1], Asa Kosto [1], Alan Lawrence [2], David Liefer [1], Michelle Lollie [1], Dominic Lucchetti [1], Nathan K. Lysne [7], Christian Lytle [1], Callum MacPherson [2], Andrew Malm [1], Spencer Mather [1], Brian Mathewson [1], Daniel Maxwell [3], Lauren McCaffrey [1], Hannah McDougall [1], Robin Mendoza [1], Michael Mills [1], Richard Morrison [2], Louis Narmour [1], Nhung Nguyen [1], Lora Nugent [1], Scott Olson [5], Daniel Ouellette [5], Jeremy Parks [1], Zach Peters [1], Jessie Petricka [1], Juan M. Pino [1], Frank Polito [1], Matthias Preidl [5], Gabriel Price [1], Timothy Proctor [8], McKinley Pugh [1], Noah Ratcliff [1], Daisy Raymondson [1], Peter Rhodes [1], Conrad Roman [1], Craig Roy [2], Ciaran Ryan-Anderson [1], Fernando Betanzo Sanchez [2], George Sangiolo [2], Tatiana Sawadski [2], Andrew Schaffer [3], Peter Schow [1], Jon Sedlacek [3], Henry Semenenko [2], Peter Shevchuk [1], Susan Shore [5], Peter Siegfried [1], Kartik Singhal [1], Seyon Sivarajah [2], Thomas Skripka [1], Lucas Sletten [3], Ben Spaun [1], R. Tucker Sprenkle [1], Paul Stoufer [1], Mariel Tader [1], Stephen F. Taylor [3], Travis H. Thompson [2], Raanan Tobey [1], Anh Tran [1], Tam Tran [1], Grahame Vittorini [3], Curtis Volin [3], Jim Walker [1], Sam White [2], Douglas Wilson [2], Quinn Wolf [1], Chester Wringe [2], Kevin Young [8], Jian Zheng [1], Kristen Zuraski [1], Charles H. Baldwin [1], Alex Chernoguzov [1], John P. Gaebler [1], Steven J. Sanders [1], Brian Neyenhuis [1], Russell Stutz [1], Justin G. Bohnet [1]

Abstract

We report on Quantinuum Helios, a 98-qubit trapped-ion quantum processor based on the quantum charge-coupled device (QCCD) architecture. Helios features $^{137}$Ba$^{+}$ hyperfine qubits, all-to-all connectivity enabled by a rotatable ion storage ring connecting two quantum operation regions by a junction, speed improvements from parallelized operations, and a new software stack with real-time compilation of dynamic programs. Averaged over all operational zones in the system, we achieve average infidelities of $2.5(1)\times10^{-5}$ for single-qubit gates, $7.9(2)\times10^{-4}$ for two-qubit gates, and $4.8(6)\times10^{-4}$ for state preparation and measurement, none of which are fundamentally limited and likely able to be improved. These component infidelities are predictive of system-level performance in both random Clifford circuits and random circuit sampling, the latter demonstrating that Helios operates well beyond the reach of classical simulation and establishes a new frontier of fidelity and complexity for quantum computers.