Author
Listed:
- E. K. Anderson
(Aarhus University)
- C. J. Baker
(Swansea University)
- W. Bertsche
(University of Manchester
Cockcroft Institute, Sci-Tech Daresbury)
- N. M. Bhatt
(Swansea University)
- G. Bonomi
(University of Brescia, Brescia and INFN Pavia)
- A. Capra
(TRIUMF)
- I. Carli
(TRIUMF)
- C. L. Cesar
(Instituto de Fisica, Universidade Federal do Rio de Janeiro)
- M. Charlton
(Swansea University)
- A. Christensen
(University of California at Berkeley)
- R. Collister
(TRIUMF
University of British Columbia)
- A. Cridland Mathad
(Swansea University)
- D. Duque Quiceno
(TRIUMF
University of British Columbia)
- S. Eriksson
(Swansea University)
- A. Evans
(TRIUMF
University of British Columbia)
- N. Evetts
(University of British Columbia)
- S. Fabbri
(University of Manchester
CERN)
- J. Fajans
(University of California at Berkeley)
- A. Ferwerda
(York University)
- T. Friesen
(University of Calgary)
- M. C. Fujiwara
(TRIUMF)
- D. R. Gill
(TRIUMF)
- L. M. Golino
(Swansea University)
- M. B. Gomes Gonçalves
(Swansea University)
- P. Grandemange
(TRIUMF)
- P. Granum
(Aarhus University)
- J. S. Hangst
(Aarhus University)
- M. E. Hayden
(Simon Fraser University)
- D. Hodgkinson
(University of Manchester
University of California at Berkeley)
- E. D. Hunter
(University of California at Berkeley)
- C. A. Isaac
(Swansea University)
- A. J. U. Jimenez
(TRIUMF)
- M. A. Johnson
(University of Manchester
Cockcroft Institute, Sci-Tech Daresbury)
- J. M. Jones
(Swansea University)
- S. A. Jones
(University of Groningen)
- S. Jonsell
(Stockholm University)
- A. Khramov
(TRIUMF
University of British Columbia
British Columbia Institute of Technology)
- N. Madsen
(Swansea University)
- L. Martin
(TRIUMF)
- N. Massacret
(TRIUMF)
- D. Maxwell
(Swansea University)
- J. T. K. McKenna
(Aarhus University
University of Manchester)
- S. Menary
(York University)
- T. Momose
(TRIUMF
University of British Columbia
University of British Columbia)
- M. Mostamand
(TRIUMF
University of British Columbia)
- P. S. Mullan
(Swansea University
ETH)
- J. Nauta
(Swansea University)
- K. Olchanski
(TRIUMF)
- A. N. Oliveira
(Aarhus University)
- J. Peszka
(Swansea University
ETH)
- A. Powell
(University of Calgary)
- C. Ø. Rasmussen
(CERN)
- F. Robicheaux
(Purdue University)
- R. L. Sacramento
(Instituto de Fisica, Universidade Federal do Rio de Janeiro)
- M. Sameed
(University of Manchester
CERN)
- E. Sarid
(Soreq NRC
Ben Gurion University)
- J. Schoonwater
(Swansea University)
- D. M. Silveira
(Instituto de Fisica, Universidade Federal do Rio de Janeiro)
- J. Singh
(University of Manchester)
- G. Smith
(TRIUMF
University of British Columbia)
- C. So
(TRIUMF)
- S. Stracka
(INFN Pisa)
- G. Stutter
(Aarhus University
University of Sussex)
- T. D. Tharp
(Marquette University)
- K. A. Thompson
(Swansea University)
- R. I. Thompson
(TRIUMF
University of Calgary)
- E. Thorpe-Woods
(Swansea University)
- C. Torkzaban
(University of California at Berkeley)
- M. Urioni
(University of Brescia, Brescia and INFN Pavia)
- P. Woosaree
(University of Calgary)
- J. S. Wurtele
(University of California at Berkeley)
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.
Suggested Citation
E. K. Anderson & C. J. Baker & W. Bertsche & N. M. Bhatt & G. Bonomi & A. Capra & I. Carli & C. L. Cesar & M. Charlton & A. Christensen & R. Collister & A. Cridland Mathad & D. Duque Quiceno & S. Erik, 2023.
"Observation of the effect of gravity on the motion of antimatter,"
Nature, Nature, vol. 621(7980), pages 716-722, September.
Handle:
RePEc:nat:nature:v:621:y:2023:i:7980:d:10.1038_s41586-023-06527-1
DOI: 10.1038/s41586-023-06527-1
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