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Observation of the effect of gravity on the motion of antimatter.
Anderson, E K; Baker, C J; Bertsche, W; Bhatt, N M; Bonomi, G; Capra, A; Carli, I; Cesar, C L; Charlton, M; Christensen, A; Collister, R; Cridland Mathad, A; Duque Quiceno, D; Eriksson, S; Evans, A; Evetts, N; Fabbri, S; Fajans, J; Ferwerda, A; Friesen, T; Fujiwara, M C; Gill, D R; Golino, L M; Gomes Gonçalves, M B; Grandemange, P; Granum, P; Hangst, J S; Hayden, M E; Hodgkinson, D; Hunter, E D; Isaac, C A; Jimenez, A J U; Johnson, M A; Jones, J M; Jones, S A; Jonsell, S; Khramov, A; Madsen, N; Martin, L; Massacret, N; Maxwell, D; McKenna, J T K; Menary, S; Momose, T; Mostamand, M; Mullan, P S; Nauta, J; Olchanski, K; Oliveira, A N; Peszka, J.
Affiliation
  • Anderson EK; Department of Physics and Astronomy, Aarhus University, Aarhus, Denmark.
  • Baker CJ; Department of Physics, Faculty of Science and Engineering, Swansea University, Swansea, UK.
  • Bertsche W; School of Physics and Astronomy, University of Manchester, Manchester, UK. william.bertsche@cern.ch.
  • Bhatt NM; Cockcroft Institute, Sci-Tech Daresbury, Warrington, UK. william.bertsche@cern.ch.
  • Bonomi G; Department of Physics, Faculty of Science and Engineering, Swansea University, Swansea, UK.
  • Capra A; University of Brescia, Brescia and INFN Pavia, Pavia, Italy.
  • Carli I; TRIUMF, Vancouver, British Columbia, Canada.
  • Cesar CL; TRIUMF, Vancouver, British Columbia, Canada.
  • Charlton M; Instituto de Fisica, Universidade Federal do Rio de Janeiro, Rio de Janeiro, Brazil.
  • Christensen A; Department of Physics, Faculty of Science and Engineering, Swansea University, Swansea, UK.
  • Collister R; Department of Physics, University of California at Berkeley, Berkeley, CA, USA.
  • Cridland Mathad A; TRIUMF, Vancouver, British Columbia, Canada.
  • Duque Quiceno D; Department of Physics and Astronomy, University of British Columbia, Vancouver, British Columbia, Canada.
  • Eriksson S; Department of Physics, Faculty of Science and Engineering, Swansea University, Swansea, UK.
  • Evans A; TRIUMF, Vancouver, British Columbia, Canada.
  • Evetts N; Department of Physics and Astronomy, University of British Columbia, Vancouver, British Columbia, Canada.
  • Fabbri S; Department of Physics, Faculty of Science and Engineering, Swansea University, Swansea, UK.
  • Fajans J; TRIUMF, Vancouver, British Columbia, Canada.
  • Ferwerda A; Department of Physics and Astronomy, University of British Columbia, Vancouver, British Columbia, Canada.
  • Friesen T; Department of Physics and Astronomy, University of British Columbia, Vancouver, British Columbia, Canada.
  • Fujiwara MC; School of Physics and Astronomy, University of Manchester, Manchester, UK.
  • Gill DR; Accelerator and Technology Sector, CERN, Geneva, Switzerland.
  • Golino LM; Department of Physics, University of California at Berkeley, Berkeley, CA, USA. joel@physics.berkeley.edu.
  • Gomes Gonçalves MB; Department of Physics and Astronomy, York University, Toronto, Ontario, Canada.
  • Grandemange P; Department of Physics and Astronomy, University of Calgary, Calgary, Alberta, Canada.
  • Granum P; TRIUMF, Vancouver, British Columbia, Canada.
  • Hangst JS; TRIUMF, Vancouver, British Columbia, Canada.
  • Hayden ME; Department of Physics, Faculty of Science and Engineering, Swansea University, Swansea, UK.
  • Hodgkinson D; Department of Physics, Faculty of Science and Engineering, Swansea University, Swansea, UK.
  • Hunter ED; TRIUMF, Vancouver, British Columbia, Canada.
  • Isaac CA; Department of Physics and Astronomy, Aarhus University, Aarhus, Denmark.
  • Jimenez AJU; Department of Physics and Astronomy, Aarhus University, Aarhus, Denmark. jeffrey.hangst@cern.ch.
  • Johnson MA; Department of Physics, Simon Fraser University, Burnaby, British Columbia, Canada.
  • Jones JM; School of Physics and Astronomy, University of Manchester, Manchester, UK.
  • Jones SA; Department of Physics, University of California at Berkeley, Berkeley, CA, USA.
  • Jonsell S; Department of Physics, University of California at Berkeley, Berkeley, CA, USA.
  • Khramov A; Department of Physics, Faculty of Science and Engineering, Swansea University, Swansea, UK.
  • Madsen N; TRIUMF, Vancouver, British Columbia, Canada.
  • Martin L; School of Physics and Astronomy, University of Manchester, Manchester, UK.
  • Massacret N; Cockcroft Institute, Sci-Tech Daresbury, Warrington, UK.
  • Maxwell D; Department of Physics, Faculty of Science and Engineering, Swansea University, Swansea, UK.
  • McKenna JTK; Van Swinderen Institute for Particle Physics and Gravity, University of Groningen, Groningen, The Netherlands.
  • Menary S; Department of Physics, Stockholm University, Stockholm, Sweden.
  • Momose T; TRIUMF, Vancouver, British Columbia, Canada.
  • Mostamand M; Department of Physics and Astronomy, University of British Columbia, Vancouver, British Columbia, Canada.
  • Mullan PS; Department of Physics, British Columbia Institute of Technology, Burnaby, British Columbia, Canada.
  • Nauta J; Department of Physics, Faculty of Science and Engineering, Swansea University, Swansea, UK.
  • Olchanski K; TRIUMF, Vancouver, British Columbia, Canada.
  • Oliveira AN; TRIUMF, Vancouver, British Columbia, Canada.
  • Peszka J; Department of Physics, Faculty of Science and Engineering, Swansea University, Swansea, UK.
Nature ; 621(7980): 716-722, 2023 Sep.
Article in En | MEDLINE | ID: mdl-37758891
ABSTRACT
Einstein's general theory of relativity from 19151 remains the most successful description of gravitation. From the 1919 solar eclipse2 to the observation of gravitational waves3, the theory has passed many crucial experimental tests. However, the evolving concepts of dark matter and dark energy illustrate that there is much to be learned about the gravitating content of the universe. Singularities in the general theory of relativity and the lack of a quantum theory of gravity suggest that our picture is incomplete. It is thus prudent to explore gravity in exotic physical systems. Antimatter was unknown to Einstein in 1915. Dirac's theory4 appeared in 1928; the positron was observed5 in 1932. There has since been much speculation about gravity and antimatter. The theoretical consensus is that any laboratory mass must be attracted6 by the Earth, although some authors have considered the cosmological consequences if antimatter should be repelled by matter7-10. In the general theory of relativity, the weak equivalence principle (WEP) requires that all masses react identically to gravity, independent of their internal structure. Here we show that antihydrogen atoms, released from magnetic confinement in the ALPHA-g apparatus, behave in a way consistent with gravitational attraction to the Earth. Repulsive 'antigravity' is ruled out in this case. This experiment paves the way for precision studies of the magnitude of the gravitational acceleration between anti-atoms and the Earth to test the WEP.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Nature Year: 2023 Type: Article Affiliation country: Denmark

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Nature Year: 2023 Type: Article Affiliation country: Denmark