This paper describes the ALPHA-2 apparatus, used at the CERN Antiproton Decelerator facility for the study of trapped antihydrogen

R. Akbari and B.X.R. Alves and C.J. Baker and M. Baquero-Ruiz and W. Bertsche and E. Butler and C. Burrows and A. Capra and C.L. Cesar and M. Charlton and R. Collister and A. Cridland and S. Eriksson and A. Evans and L.T. Evans and N. Evetts and J. Fajans and T. Friesen and M.C. Fujiwara and D.R. Gill and P. Grandemange and P. Granum and A. Gutierrez and J.S. Hangst and M.E. Hayden and D. Hodgkinson and C.A. Isaac and A. Ishida and M.A. Johnson and J.M. Jones and S.A. Jones and S. Jonsell and A. Khramov and L. Kurchaninov and A. Little and N. Madsen and D. Maxwell and J.T.K. McKenna and S

The antimatter equivalent of atomic hydrogen—antihydrogen—is an outstanding testbed for precision studies of matter–antimatter symmetry. Here we report on the simultaneous observation of both accessible hyperfine components of the 1S–2S transition in trapped antihydrogen. We determine the 2S hyperfine splitting in antihydrogen and—by comparing our results with those obtained in hydrogen—constrain the charge–parity–time-reversal symmetry-violating coefficients in the standard model extension framework.

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Baker, C. J. and Bertsche, W. and Capra, A. and Carruth, C. and Cesar, C. L. and Charlton, M. and Christensen, A. and Collister, R. and Cridland Mathad, A. and Eriksson, S. and Evans, A. and Evetts, N. and Fajans, J. and Friesen, T. and Fujiwara, M. C. and Gill, D. R. and Grandemange, P. and Granum, P. and Hangst, J. S. and Hardy, W. N. and Hayden, M. E. and Hodgkinson, D. and Hunter, E. and Isaac, C. A. and Johnson, M. A. and Jones, J. M. and Jones, S. A. and Jonsell, S. and Khramov, A. and Kurchaninov, L. and Madsen, N. and Maxwell, D. and McKenna, J. T. K. and Menary, S. and Momose, T. and

Antihydrogen is now routinely formed in ALPHA by combination of antiproton and
positron plasmas. Formed anti-atoms with energy <∼0.5 K are trapped in an octupole-
based Ioffe-Pritchard magnetic trap. Reducing trapped antihydrogen energy is expected
to increase precision in experiments that measure fundamental antihydrogen properties
for precise comparison to hydrogen. Cooling is expected to permit confinement in a

Danielle L. Hodgkinson

Antiprotons created by laser ionization of antihydrogen are observed to rapidly escape the ALPHA trap. Further, positron plasmas heat more quickly after the trap is illuminated by laser light for several hours. These phenomena can be caused by patch potentials—variations in the electrical potential along metal surfaces.

C. J. Baker, W. Bertsche, A. Capra, C. L. Cesar, M. Charlton, A. Christensen, R. Collister, A. Cridland Mathad, S. Eriksson, A. Evans, N. Evetts, J. Fajans, T. Friesen, M. C. Fujiwara, D. R. Gill, P. Grandemange, P. Granum, J. S. Hangst, M. E. Hayden, D. Hodgkinson, E. D. Hunter, C. A. Isaac, M. A. Johnson, J. Jones, S. A. Jones, S. Jonsell, A. Khramov, L. Kurchaninov, H. Landsberger, N. Madsen, D. Maxwell, J. T. K. McKenna, S. Menary, T. Momose, P. S. Mullan, J. J. Munich, K. Olchanski, A. Olin, J. Peszka, A. Powell, P. Pusa, C.Ø. Rasmussen, F. Robicheaux, R. L. Sacramento, M. Sameed, E

Support Physicist

We have laser cooled beryllium ions in a Penning-Malmberg trap dedicated for antihydrogen formation.

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Joanna Peszka

First results from ALPHA-g: Antihydrogen doesn't fall up!

Today ALPHA released the first set of results from the ALPHA-g apparatus that was added to the ALPHA setup in 2018.

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