A. Singh

Performance of the MORA Apparatus for Testing Time-Reversal Invariance in Nuclear Beta Decay

N. Goyal [1], A. Singh [1], S. Daumas-Tschopp [2], L. M. Motilla Martinez [1,3], G. Ban [2], V. Bosquet [2], J. F. Cam [2], P. Chauveau [1], S. Chinthakayala [1,3,4], G. Fremont, R. P. De Groote, F. de Oliveira Santos [1], T. Eronen [3], A. Falkowski [5,2], X. Flechard, Z. Ge [3,6,1], M. Gonzalez-Alonso, H. Guerin, L. Hayen [2], A. Jaries [3], M. Jbayli [1], A. Jokinen [3], A. Kankainen [3], B. Kootte [3], R. Kronholm [3], N. Lecesne [1], Y. Merrer [2], V. Morel [1], M. Mougeot [3], G. Neyens [4], J. Perronnel [2], M. Reponen [3], A. Raggio [3], S. Rinta-Antila [3], A. Rodriguez-Sanchez [6], N. Severijns [4], J. C. Thomas [1], C. Vandamme [2], S. Vanlangendonk [4], V. Virtanen [3,2], E. Lienard, I. D. Moore [3], P. Delahaye [1]

Abstract

The MORA experimental setup is designed to measure the triple-correlation D parameter in nuclear beta decay. The D coefficient is sensitive to possible violations of time-reversal invariance. The experimental configuration consists of a transparent Paul trap surrounded by a detection setup with alternating beta and recoil-ion detectors. The octagonal symmetry of the detection setup optimizes the sensitivity of positron-recoil-ion coincidence rates to the D correlation, while reducing systematic effects. MORA utilizes an innovative in-trap laser polarization technique. The design and performance of the ion trap, associated beamline elements, lasers and beta and recoil-ion detectors, are presented. Recent progress towards the polarization proof-of-principle is described.

Scalable hyperfine qubit state detection via electron shelving in the ${}^2$D$_{5/2}$ and ${}^2$F$_{7/2}$ manifolds in ${}^{171}$Yb$^{+}$

C. L. Edmunds [1], T. R. Tan [1], A. R. Milne [1], A. Singh [1], M. J. Biercuk [1,3], C. Hempel [1,2]

Abstract

Qubits encoded in hyperfine states of trapped ions are ideal for quantum computation given their long lifetimes and low sensitivity to magnetic fields, yet they suffer from off-resonant scattering during detection often limiting their measurement fidelity. In ${}^{171}$Yb$^{+}$ this is exacerbated by a low fluorescence yield, which leads to a need for complex and expensive hardware - a problematic bottleneck especially when scaling up the number of qubits. We demonstrate a detection routine based on electron shelving to address this issue in ${}^{171}$Yb$^{+}$ and achieve a 5.6$\times$ reduction in single-ion detection error on an avalanche photodiode to $1.8(2)\times10^{-3}$ in a 100 $μ$s detection period, and a 4.3$\times$ error reduction on an electron multiplying CCD camera, with $7.7(2)\times10^{-3}$ error in 400 $μ$s. We further improve the characterization of a repump transition at 760 nm to enable a more rapid reset of the auxiliary $^2$F$_{7/2}$ states populated after shelving. Finally, we examine the detection fidelity limit using the long-lived $^2$F$_{7/2}$ state, achieving a further 300$\times$ and 12$\times$ reduction in error to $6(7)\times10^{-6}$ and $6.3(3)\times10^{-4}$ in 1 ms on the respective detectors. While shelving-rate limited in our setup, we suggest various techniques to realize this detection method at speeds compatible with quantum information processing, providing a pathway to ultra-high fidelity detection in ${}^{171}$Yb$^{+}$.