TY - JOUR
T1 - Laser cooling of antihydrogen atoms
AU - ALPHA Collaboration
AU - Bertsche, W.
AU - Capra, A.
AU - Carruth, C.
AU - Cesar, C. L.
AU - Christensen, A.
AU - Collister, R.
AU - Mathad, April Cridland
AU - Eriksson, S.
AU - Evetts, N.
AU - Fajans, Joel
AU - Friesen, T.
AU - Fujiwara, Makoto
AU - Grandemange, P.
AU - Granum, Peter
AU - Hangst, J. S.
AU - Hardy, W. N.
AU - Hayden, M. E.
AU - Hodgkinson, D.
AU - Isaac, C. A.
AU - Jonsell, Svante
AU - Khramov, Alexander
AU - Knapp, P.
AU - Kurchaninov, L.
AU - Madsen, N.
AU - McKenna, J. T. K.
AU - Michan, J. M.
AU - Momose, T.
AU - Mullan, P. S.
AU - Munich, J. J.
AU - Olchanski, K.
AU - Olin, Arthur
AU - Peszka, Joanna
AU - Pusa, P.
AU - Rasmussen, Chris Ørum
AU - Robicheaux, F.
AU - Sacramento, R. L.
AU - Sameed, M.
AU - Sarid, E.
AU - Silveira, D. M.
N1 - Funding Information:
Acknowledgements This work was supported by: the European Research Council through its Advanced Grant programme (JSH); CNPq, FAPERJ, RENAFAE (Brazil); NSERC, CFI, NRC/TRIUMF, EHPDS/EHDRS (Canada); FNU (Nice Centre), Carlsberg Foundation (Denmark); ISF (Israel); STFC, EPSRC, the Royal Society and the Leverhulme Trust (UK); DOE, NSF (USA); and VR (Sweden). We are grateful for the efforts of the CERN AD team, without which these experiments could not have taken place. We thank P. Djuricanin (University of British Columbia) for his extensive help with the laser system. We thank J. Tonoli (CERN) and his staff as well as T. Mittertreiner (UBC) and his staff for extensive, time-critical help with machining and electrical work. We thank the staff of the Superconducting Magnet Division at Brookhaven National Laboratory for collaboration and fabrication of the trapping magnets. We are grateful to C. Marshall (TRIUMF) for his work on the ALPHA-2 cryostat. We thank F. Besenbacher (Aarhus) for timely support in procuring the ALPHA-2 external solenoid. We are grateful to T. Miller (Ohio) for advice on the initial development of the pulsed laser system. Finally, we thank M. Grant (UBC) for contributions to the laser system.
Publisher Copyright:
© 2021, The Author(s).
PY - 2021/4/1
Y1 - 2021/4/1
N2 - The photon—the quantum excitation of the electromagnetic field—is massless but carries momentum. A photon can therefore exert a force on an object upon collision 1. Slowing the translational motion of atoms and ions by application of such a force 2,3, known as laser cooling, was first demonstrated 40 years ago 4,5. It revolutionized atomic physics over the following decades 6–8, and it is now a workhorse in many fields, including studies on quantum degenerate gases, quantum information, atomic clocks and tests of fundamental physics. However, this technique has not yet been applied to antimatter. Here we demonstrate laser cooling of antihydrogen 9, the antimatter atom consisting of an antiproton and a positron. By exciting the 1S–2P transition in antihydrogen with pulsed, narrow-linewidth, Lyman-α laser radiation 10,11, we Doppler-cool a sample of magnetically trapped antihydrogen. Although we apply laser cooling in only one dimension, the trap couples the longitudinal and transverse motions of the anti-atoms, leading to cooling in all three dimensions. We observe a reduction in the median transverse energy by more than an order of magnitude—with a substantial fraction of the anti-atoms attaining submicroelectronvolt transverse kinetic energies. We also report the observation of the laser-driven 1S–2S transition in samples of laser-cooled antihydrogen atoms. The observed spectral line is approximately four times narrower than that obtained without laser cooling. The demonstration of laser cooling and its immediate application has far-reaching implications for antimatter studies. A more localized, denser and colder sample of antihydrogen will drastically improve spectroscopic 11–13 and gravitational 14 studies of antihydrogen in ongoing experiments. Furthermore, the demonstrated ability to manipulate the motion of antimatter atoms by laser light will potentially provide ground-breaking opportunities for future experiments, such as anti-atomic fountains, anti-atom interferometry and the creation of antimatter molecules.
AB - The photon—the quantum excitation of the electromagnetic field—is massless but carries momentum. A photon can therefore exert a force on an object upon collision 1. Slowing the translational motion of atoms and ions by application of such a force 2,3, known as laser cooling, was first demonstrated 40 years ago 4,5. It revolutionized atomic physics over the following decades 6–8, and it is now a workhorse in many fields, including studies on quantum degenerate gases, quantum information, atomic clocks and tests of fundamental physics. However, this technique has not yet been applied to antimatter. Here we demonstrate laser cooling of antihydrogen 9, the antimatter atom consisting of an antiproton and a positron. By exciting the 1S–2P transition in antihydrogen with pulsed, narrow-linewidth, Lyman-α laser radiation 10,11, we Doppler-cool a sample of magnetically trapped antihydrogen. Although we apply laser cooling in only one dimension, the trap couples the longitudinal and transverse motions of the anti-atoms, leading to cooling in all three dimensions. We observe a reduction in the median transverse energy by more than an order of magnitude—with a substantial fraction of the anti-atoms attaining submicroelectronvolt transverse kinetic energies. We also report the observation of the laser-driven 1S–2S transition in samples of laser-cooled antihydrogen atoms. The observed spectral line is approximately four times narrower than that obtained without laser cooling. The demonstration of laser cooling and its immediate application has far-reaching implications for antimatter studies. A more localized, denser and colder sample of antihydrogen will drastically improve spectroscopic 11–13 and gravitational 14 studies of antihydrogen in ongoing experiments. Furthermore, the demonstrated ability to manipulate the motion of antimatter atoms by laser light will potentially provide ground-breaking opportunities for future experiments, such as anti-atomic fountains, anti-atom interferometry and the creation of antimatter molecules.
UR - http://dx.doi.org/10.1038/s41586-021-03289-6
U2 - 10.1038/s41586-021-03289-6
DO - 10.1038/s41586-021-03289-6
M3 - Article
SN - 0028-0836
VL - 592
SP - 35
EP - 42
JO - Nature: international weekly journal of science
JF - Nature: international weekly journal of science
IS - 7852
ER -