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, |
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. |
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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