12 research outputs found
A reliable cw Lyman- laser source for future cooling of antihydrogen
We demonstrate a reliable continuous-wave (cw) laser source at the
1\,--2\, transition in (anti)hydrogen at 121.56\,nm (Lyman-)
based on four-wave sum-frequency mixing in mercury. A two-photon resonance in
the four-wave mixing scheme is essential for a powerful cw Lyman-
source and is well investigated.Comment: 8 pages, 3 figures, Proceedings of LEAP 201
High-power Ti:sapphire lasers for spectroscopy of antiprotonic atoms and radioactive ions
High-power Ti:sapphire lasers for spectroscopy of antiprotonic atoms and radioactive ions
Freely designable optical frequency conversion in Raman-resonant four-wave-mixing process
Two-photon laser spectroscopy of antiprotonic helium and the antiproton-to-electron mass ratio
Physical laws are believed to be invariant under the combined transformations of charge, parity and time reversal (CPT symmetry).
This implies that an antimatter particle has exactly the same mass and absolute value of charge as its particle counterpart. Metastable antiprotonic helium is a three-body atom consisting of a normal helium nucleus, an electron in its ground state and an antiproton occupying a Rydberg state with high principal and angular momentum quantum numbers, respectively n and l, such that
n~l+1 ~ 38. These atoms are amenable to precision laser spectroscopy, the results of which can in principle be used to determine the antiproton-to-electron mass ratio and to constrain the equality between the antiproton and proton charges and masses. Here we report two-photon spectroscopy of antiprotonic helium, in which two antiprotonic helium isotopes are irradiated by two counter-propagating laser beams. This excites nonlinear, two-photon transitions of the antiproton of the type (n,l) -> (n-2, l-2) at deep-ultraviolet wave-lengths (139.8, 193.0 and 197.0 nm), which partly cancel the Doppler broadening of the laser resonance caused by the thermal motion of the atoms. The resulting narrow spectral lines allowed us to measure three transition frequencies with fractional precisions of 2.3–5 parts in 10^9. By comparing the results with three-body quantum electrodynamics calculations, we derived an antiproton-to-electron mass ratio of 1,836.1526736(23), where the parenthetical
error represents one standard deviation. This agrees with the
proton-to-electron value known to a similar precision