Toward quantum sensing of electron beams using solid-state spins

J Jakob M. Grzesik (E. L. Ginzton Laboratory, Stanford University) D Dominic Catanzaro (E. L. Ginzton Laboratory, Stanford University) C Charles Roques-Carmes E Eric I. Rosenthal (E. L. Ginzton Laboratory, Stanford University) G Guido L. van de Stolpe (E. L. Ginzton Laboratory, Stanford University) A Aviv Karnieli (E. L. Ginzton Laboratory, Stanford University) G Giovanni Scuri (E. L. Ginzton Laboratory, Stanford University) S Souvik Biswas (E. L. Ginzton Laboratory, Stanford University) K Kenneth J. Leedle (E. L. Ginzton Laboratory, Stanford University) D Dylan S. Black (E. L. Ginzton Laboratory, Stanford University) R Robert L. Byer (E. L. Ginzton Laboratory, Stanford University) I Ido Kaminer (Department of Electrical and Computer Engineering, Technion-Israel Institute of Technology) R R. Joel England (SLAC National Accelerator Laboratory) S Shanhui Fan O Olav Solgaard (E. L. Ginzton Laboratory, Stanford University) J Jelena Vučković (E. L. Ginzton Laboratory, Stanford University)

Abstract

Scattering experiments with energetic particles, such as free electrons, have been historically used to reveal the quantum structure of matter. However, realizing coherent interactions between free-electron beams and solid-state quantum systems has remained out of reach, owing to their intrinsically weak coupling. Realizing such coherent control would open up opportunities for hybrid quantum platforms combining free electrons and solid-state qubits for coincident quantum information processing and nanoscale sensing. Here, we present a framework that employs negatively charged nitrogen-vacancy centers (NV − ) in diamond as quantum sensors of a bunched electron beam. We develop a Lindblad master equation description of the magnetic free-electron–qubit interactions and identify spin relaxometry as a sensitive probe of the interaction. Experimentally, we integrate a confocal fluorescence microscopy setup into a microwave-bunched electron beam line. We monitor charge-state dynamics and assess their impact on key sensing performance metrics (such as spin readout contrast), defining safe operating parameters for quantum sensing experiments. By performing T 1 relaxometry under controlled electron beam exposure, we do not resolve a measurable reduction in T 1 within experimental uncertainty, and instead establish an upper bound on the free-electron–spin coupling strength. Our results establish NV − centers as quantitative probes of free electrons, providing a metrological benchmark for free-electron–qubit coupling under realistic conditions, and chart a route toward solid-state quantum control with electron beams.

Article Details

Volume / Issue Vol. 123, Issue 25
Published June 23, 2026
ISSN 0027-8424
Publisher National Academy of Sciences

Authors (16)

J

Jakob M. Grzesik

E. L. Ginzton Laboratory, Stanford University

D

Dominic Catanzaro

E. L. Ginzton Laboratory, Stanford University

C

Charles Roques-Carmes

E

Eric I. Rosenthal

E. L. Ginzton Laboratory, Stanford University

G

Guido L. van de Stolpe

E. L. Ginzton Laboratory, Stanford University

A

Aviv Karnieli

E. L. Ginzton Laboratory, Stanford University

G

Giovanni Scuri

E. L. Ginzton Laboratory, Stanford University

S

Souvik Biswas

E. L. Ginzton Laboratory, Stanford University

K

Kenneth J. Leedle

E. L. Ginzton Laboratory, Stanford University

D

Dylan S. Black

E. L. Ginzton Laboratory, Stanford University

R

Robert L. Byer

E. L. Ginzton Laboratory, Stanford University

I

Ido Kaminer

Department of Electrical and Computer Engineering, Technion-Israel Institute of Technology

R

R. Joel England

SLAC National Accelerator Laboratory

S

Shanhui Fan

O

Olav Solgaard

E. L. Ginzton Laboratory, Stanford University

J

Jelena Vučković

E. L. Ginzton Laboratory, Stanford University