no code implementations • 8 Mar 2021 • Christophe Piveteau, David Sutter, Sergey Bravyi, Jay M. Gambetta, Kristan Temme
The Eastin-Knill theorem states that no quantum error correcting code can have a universal set of transversal gates.
Quantum Physics
no code implementations • 2 Feb 2021 • Antonio D. Corcoles, Maika Takita, Ken Inoue, Scott Lekuch, Zlatko K. Minev, Jerry M. Chow, Jay M. Gambetta
The execution of quantum circuits on real systems has largely been limited to those which are simply time-ordered sequences of unitary operations followed by a projective measurement.
Quantum Physics
no code implementations • 30 Nov 2018 • Andrew W. Cross, Lev S. Bishop, Sarah Sheldon, Paul D. Nation, Jay M. Gambetta
We introduce a single-number metric, quantum volume, that can be measured using a concrete protocol on near-term quantum computers of modest size ($n\lesssim 50$), and measure it on several state-of-the-art transmon devices, finding values as high as 8.
Quantum Physics
1 code implementation • 30 Apr 2018 • Vojtech Havlicek, Antonio D. Córcoles, Kristan Temme, Aram W. Harrow, Abhinav Kandala, Jerry M. Chow, Jay M. Gambetta
Both methods represent the feature space of a classification problem by a quantum state, taking advantage of the large dimensionality of quantum Hilbert space to obtain an enhanced solution.
18 code implementations • 11 Jul 2017 • Andrew W. Cross, Lev S. Bishop, John A. Smolin, Jay M. Gambetta
This document describes a quantum assembly language (QASM) called OpenQASM that is used to implement experiments with low depth quantum circuits.
Quantum Physics
no code implementations • 25 May 2017 • Maika Takita, Andrew W. Cross, A. D. Córcoles, Jerry M. Chow, Jay M. Gambetta
Robust quantum computation requires encoding delicate quantum information into degrees of freedom that are hard for the environment to change.
Quantum Physics
1 code implementation • 17 Apr 2017 • Abhinav Kandala, Antonio Mezzacapo, Kristan Temme, Maika Takita, Markus Brink, Jerry M. Chow, Jay M. Gambetta
Quantum computers can be used to address molecular structure, materials science and condensed matter physics problems, which currently stretch the limits of existing high-performance computing resources.
Quantum Physics Superconductivity
1 code implementation • 27 Jan 2017 • Sergey Bravyi, Jay M. Gambetta, Antonio Mezzacapo, Kristan Temme
Such encodings eliminate redundant degrees of freedom in a way that preserves a simple structure of the system Hamiltonian enabling quantum simulations with fewer qubits.
Quantum Physics
no code implementations • 1 Nov 2012 • Seth T. Merkel, Jay M. Gambetta, John A. Smolin, S. Poletto, A. D. Córcoles, B. R. Johnson, Colm A. Ryan, M. Steffen
The essential ingredient is to define a likelihood function that assumes nothing about the gates used for preparation and measurement.
Quantum Physics
no code implementations • 23 Feb 2012 • Jerry M. Chow, Jay M. Gambetta, A. D. Corcoles, Seth T. Merkel, John A. Smolin, Chad Rigetti, S. Poletto, George A. Keefe, Mary B. Rothwell, J. R. Rozen, Mark B. Ketchen, M. Steffen
We use quantum process tomography to characterize a full universal set of all-microwave gates on two superconducting single-frequency single-junction transmon qubits.
Quantum Physics Mesoscale and Nanoscale Physics
1 code implementation • 27 Jun 2011 • John A. Smolin, Jay M. Gambetta, Graeme Smith
We provide an efficient method for computing the maximum likelihood mixed quantum state (with density matrix rho) given a set of measurement outcome in a complete orthonormal operator basis subject to Gaussian noise.
Quantum Physics