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From Hydrogen to Helium+

Highly accurate tests of a theory require a system that can be both measured and calculated with extreme precision. A famous example for such a serendipitous case is two-photon spectroscopy on the 1s-2s transition in atomic hydrogen. From the theoretical point of view the hydrogen atom is a simple two body Coulomb system that can be accurately described by bound-state QED. At the same time it is experimentally well accessible because narrow band cw lasers are available for the required wavelength (243nm) and as a two-photon transition it can be excited in an inherently first-order Doppler-free configuration. This is the basis of a famous track record in physics. Over more than three decades the experimental uncertainty has improved from 10-7 in the 70ies to better than 10-14 nowadays. Theory has made remarkable process, too, and the transition frequency can be predicted to within 10-12. Unfortunately, the last decade has been sobering, since progress has stalled both theoretically and experimentally. On the experimental side it turned out to be very hard to control systematic uncertainties below a level of 10-14 in an atomic beam experiment. Theoretical predictions on the other hand require the computation of high order Feynman diagrams and used to be limited by the uncertainty of the rms charge radius of the proton. The latter enters theory only as a small correction but still contributes with the largest uncertainty. What to do?

Helium+

Spectroscopy of the 1s-2s transition in He+ offers a solution for both the experimental and theoretical challenges that are impeding progress in hydrogen 1s-2s spectroscopy. As a charged particle, He+ can be stored in the favorable environment of a Paul trap for spectroscopy. The uncertainty of the charge radius of the nucleus is far less problematic - in fact, interesting higher order QED corrections not accessible elsewhere could be determined for the first time! However, a detailed analysis shows that the experiment is not only extremely promising, but also rather challenging for several reasons: Driving the 1s-2s transition requires two XUV photons at 60.8nm where no cw lasers and refractive optics are available and light propagates in vacuum only. The best mirrors at that wavelength reflect only about 40%. Standard cooling and detection schemes fail since no cw laser is available to drive a strong cycling transition from the ground state. But albeit hard, we believe the experiment is feasible.

One of our ion traps with cooling lasers

Strategy

A careful analysis of the excitation dynamics reveals that excitation is accompanied by a significant ionization probability. We therefore plan to operate the ion trap such that the resulting He++ ions remain stored as signature for successfull excitations. We will further co-store an auxillary ion species with the He+ ions that serve as coolant (sympathetic cooling) and for detection (secular excitation). Based on the insight that frequency combs can excite two-photon transitions much like a cw laser of the same average power, we will use a high repetition rate XUV frequency comb for excitation. The XUV comb is generated by high-harmonic generation (HHG) of a NIR frequency comb. About 1µW average power focused to 1µm spot size yields an ionization rate of 1Hz.

Team

Current Members

Akira Ozawa, Fabian Schmid, Thomas Udem


Former Members

Camille Estienne, Josue Davila-Rodriguez, Guido Saathoff, Valentin Batteiger, Sebastian Knünz, Maximillian Herrmann, Jörg Robin, Fabian Alt, Frank Markert, Mariusz Semczuk


If you are considering joining our team as a Bachelor, Master or PhD student, or as a Postdoc, please email to: Thomas Udem

Further Reading

M. Herrmann, M. Haas, U.D. Jentschura, F. Kottmann, D. Leibfried, G. Saathoff, C. Gohle, A. Ozawa, V. Batteiger, S. Knünz, N. Kolachevsky, H.A. Schuessler, T.W. Hänsch and Th. Udem, Feasibility of Coherent XUV Spectroscopy on the 1s-2s Transition in singly ionized Helium, Physical Review A 79 052505 (2009)


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