Measurement of the ground state hyperfine splitting of antihydrogen

Antihydrogen is the antimatter mirror of hydrogen in which the electron is replaced by a positron and the proton by an antiproton. The ASACUSA Collaboration intends to measure the ground state hyperfine splitting of antihydrogen (the energy difference between the two states with parallel and antiparallel  electron and proton spins) at the CERN Antiproton Decelerator, with an initial precision of one part per million, to test the symmetry between matter and antimatter. The fundamental symmetry of CPT (combination of charge and parity conjugation and time reversal) predicts that matter and antimatter have equal or sign-opposite properties. However, the puzzling dominance of matter over antimatter in the universe warrants precise measurements of antimatter properties - such as the transition frequencies in antihydrogen atoms - to compare with their matter counterparts. In fact, theories beyond the so far well established Standard Model (such as string theory) predict a violation of the CPT symmetry at some level.

Antihydrogen is the simplest stable atom composed solely of antimatter, and hydrogen is one of the most precisely studied atomic systems. The hydrogen ground state hyperfine splitting of about 1.42 GHz had been measured earlier very accurately by a maser experiment with a relative precision of about 1 part in 1012. It was also determined recently by ASACUSA, albeit with a more modest precision of a few parts per billion (ref.1) in a hydrogen beam by using the Rabi resonance method, which we will also apply to determine the hyperfine transition frequency of antihydrogen.

Figure 1 shows the behaviour of the two hyperfine states of antihydrogen which split to four when switching an external magnetic field (Breit-Rabi diagram). The total angular momentum F and its pro- jection M on the quantisation axis are given. With ASACUSA’s setup two transitions, σ1 and π1, are accessible. The hyperfine transition frequency can then be determined by measuring one of the transitions at several field strengths and extrapolating to zero field.

Figure 1: Breit-Rabi diagram showing the magnetic field dependence of the four hyperfine states of antihydrogen.


Figure 2: Sketch of the apparatus to measure the ground state hyperfine structure of antihydrogen; 1: 22Na-source, 2: e+- accumulator, 3: e+ transport line, 4: MUSASHI trap, 5: double CUSP, 6: field ionizer, 7: microwave cavity, 8: sextupole magnet,
9: antihydrogen detector.


Figure 2 shows a sketch of the experimental setup: Antiprotons are stored in the MUSASHI trap (ref. 2). Positrons are obtained from a 22Na source and stored in the positron accumulator. Together they form antihydrogen in the double CUSP mixing trap (figure 3). The neutral antihydrogen atoms escape the trap and get spin polarised by the strong magnetic field gradients of the CUSP trap. Low-field seekers enter the spectrometer consisting of a microwave cavity - to induce hyperfine transitions - and an analysing sextupole magnet.

The force from magnetic field gradients exerted on the magnetic moments separates the antihydrogen atoms according to their spin states (Stern-Gerlach effect), the sextupole magnet focusing the low-field seeking states and defocusing the high-field seekers. A detector (ref. 5) records the annihilation signal at the end of the beamline, as a function of microwave frequency. The first antihydrogen beam was produced by ASACUSA in 2012 (ref. 3).





Figure 3: Double CUSP trap made of two sets of anti-Helmholtz coils which trap antiprotons and positrons, and magnetic field dependence along the axis. Antihydrogen is produced by injecting the antiprotons into the positron plasma. The upstream potential barrier closes the trap from which only neutral antihydrogen atoms can escape. For details see ref. 4.

References:

1. M. Diermaier et al., Nature Communications 8 (2017) 1
2. N. Kuroda et al., Phys. Rev. ST Accel. Beams 15 (2012) 024702

3. N. Kuroda et al., Nature Communications 5 (2014) 3089
4. M. Tajima et al., J. Instrumentation 14 (2019) P05009
5. C. Sauerzopf
et al., Nucl. Instr. Meth.  in Phys. Res. A845 (2017) 579

See also: "A source of antihydrogen for in-flight hyperfine spectroscopy"
Nat. Commun. 5 (2014) 3089
.
https://www.nature.com/articles/ncomms4089

Useful links:

ASACUSA trap group (MUSASHI) (RIKEN, U-Tokyo group)

Hbar-Hfs - hyperfine structure of Antihydrogen (Vienna group)

In-beam hyperfine spectroscopy of hydrogen and antihydrogen (poster)

Measurements of the Principal Quantum Number Distribution in a Beam of Antihydrogen Atoms

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* Spokesman

CA 4.2.2023