<p>The hydrogen atom is a touchstone for the foundations, evolution and frontiers of quantum theory<sup><CitationRef AdditionalCitationIDS="CR2 CR3 CR4 CR5 CR6 CR7 CR8" CitationID="CR1">1</CitationRef>–<CitationRef CitationID="CR9">9</CitationRef></sup>. Key spectral lines of this atom have been determined to remarkable precision<sup><CitationRef CitationID="CR10">10</CitationRef>,<CitationRef CitationID="CR11">11</CitationRef></sup>. Our research focuses on the study of antihydrogen, the antimatter counterpart of hydrogen. We test fundamental symmetries of nature (such as simultaneous charge conjugation, parity inversion, and time reversal or CPT symmetry) through precision comparisons of these atomic systems<sup><CitationRef CitationID="CR12">12</CitationRef></sup>. Recent 1S–2S spectroscopic measurements on trapped antihydrogen have achieved relative precisions of parts per trillion (refs. <sup><CitationRef CitationID="CR13">13</CitationRef>,<CitationRef CitationID="CR14">14</CitationRef></sup>). However, the ground-state hyperfine splitting, which is sensitive to the internal structure of the antiproton, has only been measured to 400 parts per million (ppm). Here we report a 4 ppm measurement of the antihydrogen ground-state hyperfine splitting energy <i>a</i><sub>1S</sub>, advancing the state-of-the-art precision<sup><CitationRef CitationID="CR15">15</CitationRef></sup> by two orders of magnitude. From microwave spectroscopy experiments with roughly 24,000 anti-atoms, we determine <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({a}_{1{\rm{S}}}/h=\mathrm{1,420,404.8}\pm 1.1(\mathrm{stat.})\pm 5.6\,(\mathrm{sys.})\,\text{kHz}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>a</mi> <mrow> <mn>1</mn> <mi mathvariant="normal">S</mi> </mrow> </msub> <mo>/</mo> <mi>h</mi> <mo>=</mo> <mn>1,420,404.8</mn> <mo>±</mo> <mn>1.1</mn> <mo>(</mo> <mi>stat.</mi> <mo>)</mo> <mo>±</mo> <mn>5.6</mn> <mspace width="0.25em" /> <mo>(</mo> <mi>sys.</mi> <mo>)</mo> <mspace width="0.25em" /> <mtext>kHz</mtext> </math></EquationSource> </InlineEquation> in a 1-T magnetic field, consistent with expectations for hydrogen<sup><CitationRef CitationID="CR11">11</CitationRef></sup>. At this level, our measurement is sensitive to the internal structure of the antiproton, which contributes at about 40 ppm and is approaching the limit of existing theoretical analyses<sup><CitationRef CitationID="CR16">16</CitationRef></sup>. The gains we report are the product of marked advances in magnetic trap field control, stabilization and characterization; anti-atom spin-state manipulation; and improved antihydrogen accumulation rate<sup><CitationRef CitationID="CR17">17</CitationRef></sup>.</p>

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Four ppm measurement of the antihydrogen ground-state hyperfine splitting

  • R. Akbari,
  • L. O. de Araujo Azevedo,
  • C. J. Baker,
  • W. Bertsche,
  • N. M. Bhatt,
  • G. Bonomi,
  • A. Capra,
  • I. Carli,
  • C. L. Cesar,
  • M. Charlton,
  • A. Cridland Mathad,
  • A. Del Vincio,
  • D. Duque Quiceno,
  • S. Eriksson,
  • A. Evans,
  • J. Fajans,
  • T. Friesen,
  • M. C. Fujiwara,
  • L. M. Golino,
  • M. B. Gomes Gonçalves,
  • J. S. Hangst,
  • M. E. Hayden,
  • P. Heidari,
  • D. Hodgkinson,
  • C. A. Isaac,
  • S. A. Jones,
  • S. Jonsell,
  • N. Madsen,
  • V. R. Marshall,
  • J. T. K. McKenna,
  • T. Momose,
  • J. Nauta,
  • A. N. Oliveira,
  • A. Powell,
  • C. Ø. Rasmussen,
  • T. Robertson-Brown,
  • F. Robicheaux,
  • R. L. Sacramento,
  • E. Sarid,
  • J. Schoonwater,
  • D. M. Silveira,
  • J. Singh,
  • G. Smith,
  • C. So,
  • S. Stracka,
  • J. Suh,
  • A. G. Swadling,
  • T. D. Tharp,
  • K. A. Thompson,
  • R. I. Thompson,
  • E. Thorpe-Woods,
  • A. J. Uribe Jimenez,
  • M. Urioni,
  • D. P. van de Werf,
  • S. G. Wilson,
  • P. Woosaree,
  • J. S. Wurtele,
  • C. L. Cesar,
  • A. Del Vincio,
  • D. P. van de Werf

摘要

The hydrogen atom is a touchstone for the foundations, evolution and frontiers of quantum theory19. Key spectral lines of this atom have been determined to remarkable precision10,11. Our research focuses on the study of antihydrogen, the antimatter counterpart of hydrogen. We test fundamental symmetries of nature (such as simultaneous charge conjugation, parity inversion, and time reversal or CPT symmetry) through precision comparisons of these atomic systems12. Recent 1S–2S spectroscopic measurements on trapped antihydrogen have achieved relative precisions of parts per trillion (refs. 13,14). However, the ground-state hyperfine splitting, which is sensitive to the internal structure of the antiproton, has only been measured to 400 parts per million (ppm). Here we report a 4 ppm measurement of the antihydrogen ground-state hyperfine splitting energy a1S, advancing the state-of-the-art precision15 by two orders of magnitude. From microwave spectroscopy experiments with roughly 24,000 anti-atoms, we determine \({a}_{1{\rm{S}}}/h=\mathrm{1,420,404.8}\pm 1.1(\mathrm{stat.})\pm 5.6\,(\mathrm{sys.})\,\text{kHz}\) a 1 S / h = 1,420,404.8 ± 1.1 ( stat. ) ± 5.6 ( sys. ) kHz in a 1-T magnetic field, consistent with expectations for hydrogen11. At this level, our measurement is sensitive to the internal structure of the antiproton, which contributes at about 40 ppm and is approaching the limit of existing theoretical analyses16. The gains we report are the product of marked advances in magnetic trap field control, stabilization and characterization; anti-atom spin-state manipulation; and improved antihydrogen accumulation rate17.