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arXiv:1003.0622 · Hyperfine Interactions

Longitudinal atomic beam spin echo experiments: a possible way to study parity violation in hydrogen

Maarten DeKieviet, Thomas Gasenzer, Otto Nachtmann, Martin-Isbjörn Trappe

Published May 26, 2011• 5 citations
arXivHTMLPDF
DOI
10.1007/s10751-011-0276-x

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We present a nonrelativistic theory for the quantum mechanical description of longitudinal atomic beam spin echo experiments, where a beam of neutral atoms is subjected to static electric and magnetic fields. The atomic wave function is the solution of a matrix-valued Schroedinger equation and can be written as superposition of local (atomic) eigenstates of the potential matrix. The position- and time-dependent amplitude function of each eigenstate represents an atomic wave packet and can be calculated in a series expansion with a master formula that we derive. The zeroth order of this series expansion describes the adiabatic limit, whereas the higher order contributions contain the mixing of the eigenstates and the corresponding amplitude functions. We give a tutorial for the theoretical description of longitudinal atomic beam spin echo experiments and for the so-called Fahrplan model, which is a visualisation tool for the propagation of wave packets of different atomic eigenstates. As an example for the application of our theory, we study parity violating geometric (Berry-)phases. In this context, we define geometric flux densities, which for certain field configurations can be used to illustrate geometric phases in a vector diagram. Considering an example with a specific field configuration, we prove the existence of a parity violating geometric phase.

arXiv:0705.2508•May 17, 2007•0 citations
In the present thesis Berry phases for metastable states of hydrogen and helium exposed \nto external electromagnetic fields are investigated. One main goal is the derivation of \na parity-violating observable incorporating the electroweak mixing angle. The study is \ndone in view of an available high-precision atomic beam spin echo interferometer and \nwith respect to the theoretically very well-known structure of hydrogen. We determine \nthe general properties of parity-violating and parity-conserving Berry phases and their \nflux-density vector fields distinguished by their behaviour under proper and improper \nrotations. This allows for extensive analytical investigations and cross-checks of our \nnumerical computations. Regarding hydrogen, we reveal geometry-dependent modifications \nof atomic lifetimes due to parity-conserving imaginary Berry phases. Deriving \nthe evolution of the atomic wave packets, we establish the theoretical description of an \natom interferometer. An analytical expression for the spin echo signal, easily accessible \nin experiment, is presented and numerically evaluated to extract parity-violating \nsignals. We discuss the implications of the computed parity-violating effects on interferometric \nprecision measurements of the proton’s weak charges. Moreover, we outline \nthe concept of Heisenberg-limited atom interferometry to improve the resolution for \nmeasurements of Berry phases. Finally, we present predictions for parity-conserving \nBerry phases of metastable helium states studied in the Heidelberg experiment.
We present a nonrelativistic theory for the quantum mechanical description of longitudinal atomic beam spin echo experiments, where a beam of neutral atoms is subjected to static electric and magnetic fields. The atomic wave function is the solution of a matrix-valued Schroedinger equation and can be written as superposition of local (atomic) eigenstates of the potential matrix. The position- and time-dependent amplitude function of each eigenstate represents an atomic wave packet and can be calculated in a series expansion with a master formula that we derive. The zeroth order of this series expansion describes the adiabatic limit, whereas the higher order contributions contain the mixing of the eigenstates and the corresponding amplitude functions. We give a tutorial for the theoretical description of longitudinal atomic beam spin echo experiments and for the so-called Fahrplan model, which is a visualisation tool for the propagation of wave packets of different atomic eigenstates. As an example for the application of our theory, we study parity violating geometric (Berry-)phases. In this context, we define geometric flux densities, which for certain field configurations can be used to illustrate geometric phases in a vector diagram. Considering an example with a specific field configuration, we prove the existence of a parity violating geometric phase.