A femtosecond optical frequency comb and continuous-wave pulse-amplified laser were used to measure 12 transition frequencies of antiprotonic helium to fractional precisions of 9-16 10 ÿ9 . One of these is between two states having microsecond-scale lifetimes hitherto unaccessible to our precision laser spectroscopy method. Comparisons with three-body QED calculations yielded an antiproton-to-electron mass ratio of M p =m e 1836:152 6745. DOI: 10.1103/PhysRevLett.96.243401 PACS numbers: 36.10.ÿk, 06.20.Dk, 14.20.Dh, 32.70.Jz We report here new measurements on the transition frequencies of antiprotonic helium atoms ( pHe e ÿ ÿ p ÿ 4 He 2 ) [1] using a femtosecond optical frequency comb [2,3] in conjunction with a continuous-wave (cw) pulse-amplified laser (Fig. 1). Their experimental precision is a factor 6 -20 better than our previous best ones [4], and now approaches those of, e.g., the 1 1 s-2 1 s [5] and 1 1 s-2 1 p [6] transitions in ordinary helium. From the frequencies of 12 transitions measured to the Doppler-broadened limit at a cryogenic temperature of 10 K, we have deduced the mass and charge of the antiproton relative to both the proton and the electron with a precision of the order of the known proton-to-electron mass ratio [7].Reference [4] describes how a radio-frequency quadrupole decelerator was used to slow down the antiprotons emerging from the CERN Antiproton Decelerator to 100-keV energies. They were then stopped in a helium target of low atomic density 10 18 cm ÿ3 to produce pHe atoms which filled a volume V 100 cm 3 . Antiprotons in pHe states with high principal (n 38) and angular momentum (') quantum numbers reach the helium nucleus over a period of several microseconds. The resulting delayed annihilation time spectra (DATS), i.e., the annihilation rate versus time elapsed since pHe formation, was measured by Cherenkov counters [ Fig. 2(a)]. In all but one of the present experiments, linearly polarized laser pulses of energy density " 0:04-1 mJ=cm 2 (e.g., applied here at t 1 s) stimulated transitions with dipole moments 0.02 -0.3 D from these pHe states, to states with nanosecond-scale lifetimes against Auger emission [1] and annihilation. The resulting peak in the DATS signaled the resonant frequency.Only pulsed lasers can provide the megawatt-scale intensities needed here to induce the pHe transitions. However, fluctuations in their frequency and linewidth and the difficulty of calibrating the wide range of pHe wavelengths 264:7-726:1 nm have so far limited our experimental precision [4]. We have now circumvented these problems by basing our experiments on a cw laser whose frequency cw could be stabilized with a precision <4 10 ÿ10 against an optical comb. Its intensity was then amplified [6,8,9] by a factor 10 6 to produce a pulsed laser beam of frequency pl cw with an accuracy and resolution 1-2 orders of magnitude higher than before [4].This was done as follows: First, a Nd:YVO 4 laser (Coherent Verdi, B in Fig. 1

Antihydrogen, a positron bound to an antiproton, is the simplest antiatom. Its counterpart—hydrogen—is one of the most precisely investigated and best understood systems in physics research. High-resolution comparisons of both systems provide sensitive tests of CPT symmetry, which is the most fundamental symmetry in the Standard Model of elementary particle physics. Any measured difference would point to CPT violation and thus to new physics. Here we report the development of an antihydrogen source using a cusp trap for in-flight spectroscopy. A total of 80 antihydrogen atoms are unambiguously detected 2.7 m downstream of the production region, where perturbing residual magnetic fields are small. This is a major step towards precision spectroscopy of the ground-state hyperfine splitting of antihydrogen using Rabi-like beam spectroscopy.

We report here the first successful synthesis of cold antihydrogen atoms employing a cusp trap, which consists of a superconducting anti-Helmholtz coil and a stack of multiple ring electrodes. This success opens a new path to make a stringent test of the CPT symmetry via high precision microwave spectroscopy of ground-state hyperfine transitions of antihydrogen atoms.