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An experimental limit on the charge of antihydrogen.
- Amole, C;
- Ashkezari, MD;
- Baquero-Ruiz, M;
- Bertsche, W;
- Butler, E;
- Capra, A;
- Cesar, CL;
- Charlton, M;
- Eriksson, S;
- Fajans, J;
- Friesen, T;
- Fujiwara, MC;
- Gill, DR;
- Gutierrez, A;
- Hangst, JS;
- Hardy, WN;
- Hayden, ME;
- Isaac, CA;
- Jonsell, S;
- Kurchaninov, L;
- Little, A;
- Madsen, N;
- McKenna, JTK;
- Menary, S;
- Napoli, SC;
- Nolan, P;
- Olchanski, K;
- Olin, A;
- Povilus, A;
- Pusa, P;
- Rasmussen, CØ;
- Robicheaux, F;
- Sarid, E;
- Silveira, DM;
- So, C;
- Tharp, TD;
- Thompson, RI;
- van der Werf, DP;
- Vendeiro, Z;
- Wurtele, JS;
- Zhmoginov, AI;
- Charman, AE
- et al.
Published Web Location
https://doi.org/10.1038/ncomms4955Abstract
The properties of antihydrogen are expected to be identical to those of hydrogen, and any differences would constitute a profound challenge to the fundamental theories of physics. The most commonly discussed antiatom-based tests of these theories are searches for antihydrogen-hydrogen spectral differences (tests of CPT (charge-parity-time) invariance) or gravitational differences (tests of the weak equivalence principle). Here we, the ALPHA Collaboration, report a different and somewhat unusual test of CPT and of quantum anomaly cancellation. A retrospective analysis of the influence of electric fields on antihydrogen atoms released from the ALPHA trap finds a mean axial deflection of 4.1 ± 3.4 mm for an average axial electric field of 0.51 V mm(-1). Combined with extensive numerical modelling, this measurement leads to a bound on the charge Qe of antihydrogen of Q=(-1.3 ± 1.1 ± 0.4) × 10(-8). Here, e is the unit charge, and the errors are from statistics and systematic effects.
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