Y. Jones-Alberty

collaborators

3 papers

nucl-ex2026

Differential cross sections for $^{12} C (n, I^\pm_{0})$ , $^{16} O (n, I^\pm_{0})$ and $^{16} O (n, I^\pm_{1, 2, 3})$ between $E_{n}$ = 7.2 and 10 MeV with an active-target Time Projection Chamber

J. Bishop, C. E. Parker, R. Smith +24

Data for the $^{12} C (n, I^\pm_{0})$ , $^{16} O (n, I^\pm_{0})$ and $^{16} O (n, I^\pm_{1, 2, 3})$ differential cross sections are important for several differen…

quant-ph2026

Characterization of Radiation-Induced Errors in Superconducting Qubits Protected with Various Gap-Engineering Strategies

H. Douglas Pinckney, Thomas McJunkin, Alan W. Hunt +26

Impacts from high-energy particles cause correlated errors in superconducting qubits by increasing the quasiparticle density in the vicinity of the Josephson junctions (JJs). Such…

quant-ph2026

On-Demand Correlated Errors in Superconducting Qubits from a Particle Accelerator

Thomas McJunkin, A. W. Hunt, Yenuel Jones-Alberty +9

Ionizing radiation is a known source of correlated errors in superconducting quantum processors, inhibiting the functionality of quantum error correction surface codes. High-energy…

Differential cross sections for 12C(n,I^±0​), 16O(n,I^±0​) and 16O(n,I^±1,2,3​) between En​ = 7.2 and 10 MeV with an active-target Time Projection Chamber

Characterization of Radiation-Induced Errors in Superconducting Qubits Protected with Various Gap-Engineering Strategies

On-Demand Correlated Errors in Superconducting Qubits from a Particle Accelerator

Differential cross sections for $^{12} C (n, I^\pm_{0})$ , $^{16} O (n, I^\pm_{0})$ and $^{16} O (n, I^\pm_{1, 2, 3})$ between $E_{n}$ = 7.2 and 10 MeV with an active-target Time Projection Chamber