Grahame Vittorini

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.

Scalable Multispecies Ion Transport in a Grid-Based Surface-Electrode Trap

Robert D. Delaney [1], Lucas R. Sletten [2], Matthew J. Cich [2], Brian Estey [1], Maya I. Fabrikant [1], David Hayes [1], Ian M. Hoffman [1], James Hostetter [2], Christopher Langer [1], Steven A. Moses [1], Abigail R. Perry [1], Timothy A. Peterson [2], Andrew Schaffer [2], Curtis Volin [1], Grahame Vittorini [2], William Cody Burton [1]

Abstract

Quantum processors based on linear arrays of trapped ions have achieved exceptional performance, but scaling to large qubit numbers requires realizing two-dimensional ion arrays as envisioned in the quantum charge-coupled device (QCCD) architecture. Here we present a scalable method for the control of ion crystals in a grid-based surface-electrode Paul trap and characterize it in the context of transport operations that sort and reorder multispecies crystals. By combining cowiring of control electrodes at translationally symmetric locations in each grid site with the sitewise ability to exchange the voltages applied to two special electrodes gated by a binary input, site dependent operations can be achieved using only a fixed number of analog voltage signals and a single digital input per site. In two separate experimental systems containing nominally identical grid traps, one using $^{171}\mathrm{Yb}^{+}$-$^{138}\mathrm{Ba}^{+}$ crystals and the other $^{137}\mathrm{Ba}^{+}$-$^{88}\mathrm{Sr}^{+}$, we demonstrate this method by characterizing the conditional intrasite crystal reorder and the conditional exchange of ions between adjacent sites on the grid. Averaged across a multisite region of interest, we measure subquanta motional excitation in the axial in-phase and out-of-phase modes of the crystals following these operations at exchange rates of 2.5 kHz. In this initial demonstration, the logic controlling the voltage exchange occurs in software, but the applied signals mimic a proposed hardware implementation using crossover switches. These techniques can be further extended to implement other conditional operations in the QCCD architecture such as gates, initialization and measurement.

High fidelity state preparation and measurement of ion hyperfine qubits with I > 1/2

Fangzhao Alex An [1], Anthony Ransford [2], Andrew Schaffer [1], Lucas R. Sletten [1], John Gaebler [2], James Hostetter [1], Grahame Vittorini [1]

Abstract

We present a method for achieving high fidelity state preparation and measurement (SPAM) using trapped ion hyperfine qubits with nuclear spins higher than $I = 1/2$. The ground states of these higher nuclear spin isotopes do not afford a simple frequency-selective state preparation scheme. We circumvent this limitation by stroboscopically driving strong and weak transitions, blending fast optical pumping using dipole transitions and narrow microwave or optical quadrupole transitions. We demonstrate this method with the $I=3/2$ isotope $^{137}\mbox{Ba}^+$ to achieve a SPAM infidelity of $\left(9.0 \pm 1.3\right) \times 10^{-5}$ ($-40.5 \pm 0.6$ dB), facilitating the use of a wider range of ion isotopes with favorable wavelengths and masses for quantum computation.

Modulating carrier and sideband coupling strengths in a standing wave gate beam

Thomas E. deLaubenfels [1,2], Karl A. Burkhardt [3], Grahame Vittorini [2], J. True Merrill [1], Kenneth R. Brown [3,2,4], Jason M. Amini [1]

Abstract

We control the relative coupling strength of carrier and first order motional sideband interactions of a trapped ion by placing it in a resonant optical standing wave. Our configuration uses the surface of a microfabricated chip trap as a mirror, avoiding technical challenges of in-vacuum optical cavities. Displacing the ion along the standing wave, we show a periodic suppression of the carrier and sideband transitions with the cycles for the two cases $180^\circ$ out of phase with each other. This technique allows for suppression of off-resonant carrier excitations when addressing the motional sidebands, with applications in quantum simulation and quantum control. Using the standing wave fringes, we measure the relative ion height as a function of applied electric field, allowing for a precise measurement of ion displacement and, combined with measured micromotion amplitudes, a validation of trap numerical models.

Modular cryostat for ion trapping with surface-electrode ion traps

Grahame Vittorini [1], Kenneth Wright [2], Kenneth R. Brown [1], Alexa W. Harter [2], S. Charles Doret [2]

Abstract

We present a simple cryostat purpose built for use with surface-electrode ion traps, designed around an affordable, large cooling power commercial pulse tube refrigerator. A modular vacuum enclosure with a single vacuum space facilitates interior access, and enables rapid turnaround and flexiblity for future modifications. Long rectangular windows provide nearly 360 degrees of optical access in the plane of the ion trap, while a circular bottom window near the trap enables NA 0.4 light collection without the need for in-vacuum optics. We evaluate the system's mechanical and thermal characteristics, and we quantify ion trapping performance by trapping 40Ca+, finding small stray electric fields, long ion lifetimes, and low ion heating rates.