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The new beam profile measurement for the Antiproton Decelerator (AD) at CERN is based on a single Gas Electron Multiplier (GEM) with a 2D readout structure. This detector is very light, ~0.4% X_0, as required by the low energy of the…

Instrumentation and Detectors · Physics 2012-08-31 Serge Duarte Pinto , Philippe Carrière , Jens Spanggaard , Gerard Tranquille

We present measurements of hyperfine structure (HFS) of the $nP_J$ Rydberg states for large principal quantum number $n$ range ($n=41-55$) employing the microwave spectroscopy in an ultra-cold cesium Rydberg ensemble. A microwave field with…

Atomic Physics · Physics 2024-10-15 Rong Song , Jingxu Bai , Zhenhua Li , Yuechun Jiao , Suotang Jia , Jianming Zhao

A hydrogen-like atom consisting of a positive muon and an electron is known as muonium. It is a near-ideal two-body system for a precision test of bound-state theory and fundamental symmetries. The MuSEUM collaboration performed a new…

Positronium is an ideal system for the research of the QED, especially for the QED in bound state. The discrepancy of 3.9\sigma is found recently between the measured HFS values and the QED prediction ($O(\alpha^3)$). It might be due to the…

High Energy Physics - Experiment · Physics 2015-03-13 S. Asai , T. Suehara , T. Yamazaki , G. Akimoto , A. Miyazaki , T. Namba , T. Kobayashi , H. Saito , T. Idehara , I. Ogawa , Y. Urishizaki , S. Sabchevski

Accurate spectroscopic investigations of the heaviest elements are inherently challenging, due to their short lifetimes and low production yields. Success of such measurements requires both dedicated experimental techniques and strong…

A consistent quantum mechanical calculation of partial cross-sections leading to different final states of antiprotonic helium atom was performed. For the four-body scattering wave function, corresponding to the initial state, as well as…

Atomic Physics · Physics 2007-05-23 J. Revai , N. V. Shevchenko

Antiprotons are produced at CERN by colliding a 26 GeV/c proton beam with a fixed target made of a 3 mm diameter, 55 mm length iridium core. The inherent characteristics of antiproton production involve extremely high energy depositions…

Instrumentation and Detectors · Physics 2018-08-22 Claudio Torregrosa Martin , Antonio Perillo-Marcone , Marco Calviani , José-Luis Muñoz-Cobo

This paper discusses the first observation of stimulated magnetic resonance transitions between the hyperfine levels of trapped ground state atomic antihydrogen, confirming its presence in the ALPHA apparatus. Our observations show that…

High Energy Physics - Experiment · Physics 2019-09-04 Arthur Olin

The hyperfine structure of the ground state of erbium doped yttrium orthosilicate is analyzed with the use of electron paramagnetic resonance experiments in a tunable microwave resonator. This work was prompted by the disagreement between…

Both the 1S-2S transition and the ground state hyperfine spectrum have been observed in trapped antihydrogen. The former constitutes the first observation of resonant interaction of light with an anti-atom, and the latter is the first…

Atomic Physics · Physics 2018-03-28 S. Eriksson

Very accurate transition frequencies of HC$_5$N were determined between 5.3 and 21.4 GHz with a Fourier transform microwave spectrometer. The molecules were generated by passing a mixture of HC$_3$N and C$_2$H$_2$ highly diluted in neon…

Instrumentation and Methods for Astrophysics · Physics 2020-06-22 Thomas F. Giesen , Michael E. Harding , Jürgen Gauss , Jens-Uwe Grabow , Holger S. P. Müller

Numerical ab initio variational calculations of the transition probabilities and ac Stark shifts in two-photon transitions of antiprotonic helium atoms driven by two counter-propagating laser beams are presented. We found that sub-Doppler…

Atomic Physics · Physics 2010-06-30 Masaki Hori , Vladimir I. Korobov

A measurement of the hyperfine coefficients and isotope shifts for the Dy I 421.291 nm transition [$4f^{10}6s^2 (J=8)\to4f^{10}6s6p (J=9)$] using atomic beam laser-induced fluorescence spectroscopy is presented. A King Plot analysis is…

Atomic Physics · Physics 2015-05-13 N. Leefer , A Cingöz , D. Budker

The production of antihydrogen in flight in antiproton-nucleus collisions is calculated theoretically in the Plane Wave Born Approximation (which is equivalent to the straight line semiclassical approximation). Antihydrogen has been…

High Energy Physics - Phenomenology · Physics 2009-10-30 C. A. Bertulani , G. Baur

We perform the four-body calculation of the hyperfine structure in the first rotational state $J=1$ of the H$_2$, D$_2$, and HD molecules and determine the accurate value for the deuteron electric quadrupole moment $Q_d =…

Chemical Physics · Physics 2021-01-04 Mariusz Puchalski , Jacek Komasa , Krzysztof Pachucki

We demonstrate a technique to measure hyperfine structure using a frequency-stabilized diode laser and an acousto-optic modulator locked to the frequency difference between two hyperfine peaks. We use this technique to measure hyperfine…

Atomic Physics · Physics 2007-05-23 Umakant D. Rapol , Anusha Krishna , Vasant Natarajan

We present improved theoretical calculations of transition frequencies for the fundamental transitions $(L\!=\!0,v\!=\!1)\to(L'\!=\!0,v'\!=\!0)$ in the hydrogen molecular ions H$_2^+$ and HD$^+$ with a relative uncertainty $4\cdot10^{-11}$…

Atomic Physics · Physics 2017-02-20 V. I. Korobov , L. Hilico , J. -P. Karr

Measurements of the longitudinal structure function FL at the ep collider HERA are presented. They are derived from inclusive deep inelastic neutral current e+p scattering cross section measurements based on data collected in 2007 with the…

High Energy Physics - Experiment · Physics 2008-10-29 Vladimir Chekelian

We report on the improved measurement of the hyperfine structure of $4f^{12}(^3 H_6)5d_{5/2}6s^2$ $(J=9/2)$ excited state in Tm-169 which is involved in the second-stage laser cooling of Tm. To measure the absolute value of the hyperfine…