Special issue on antihydrogen and positronium
Special issue on antihydrogen and positronium
复制标题
反氢和正电子号特刊
DOI:
10.1088/1361-6455/aa75d8
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发表时间:
2017
期刊:
影响因子:
--
通讯作者:
Charlton M
中科院分区:
文献类型:
--
作者:
Charlton M
Since its prediction and discovery nearly 90 years ago, the positron (e+) has been the object of fascination, exploration, manipulation and application. Its arrival, when Dirac first successfully united quantum mechanics with special relativity [1], ushered in a new era in physics in which it became important to understand particles (including those comprised of antimatter) and their interactions, and the symmetries that underpin their nature and behaviour. Advances over many years in particle physics led to the development of the so-called Standard Model in which the role of antimatter is innate.What this model tells us is that the properties of particles and antiparticles should either be identically equal, or equal but opposite. Thus, the positron and the electron (e-) should have the same rest mass, but opposite charge. Furthermore, composite antimatter systems, such as the antiproton, p, should have properties similarly related to those of the proton (p) whilst atoms and anti-atoms (and here we are principally concerned with hydrogen, H, and antihydrogen, H) should have, for instance, identical spectral properties. And so far, whenever we have checked, we have found these symmetries to be obeyed to the measurement precision (see, eg,[2] for a recent review). However, behind this cosy understanding lies a puzzle. The standard model, our best theory of particle physics, cannot explain why the universe appears to be almost devoid of antimatter. An equivalent expression of this is that we do not understand why there is a material universe for us to observe and inhabit, since the matter and antimatter created in the big bang should have (almost) completely mutually annihilated leaving a universe comprised mainly of photons. That this is clearly not the case is a major motivation for many current particle physics investigations, and it provides one of the bases for the study of H. That an e+–e− bound state could exist was pointed out shortly after the discovery of the positron [3], and was soon known as positronium, Ps [4]. Interest awoke with its discovery and the ensuing seminal investigations of some of its properties by Deutsch and co-workers [5–7]. A major motivation for the study of Ps is that it is the paradigm system for bound state quantum electrodynamics (QED) since there are no hadronic complications due to the structure of heavier
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DOI:
10.1088/0953-4075/49/6/064002
发表时间:
2016
期刊:
Journal of Physics B: Atomic, Molecular and Optical Physics
影响因子:
--
作者:
R. McConnell;G. Gabrielse;W. Kolthammer;P. Richerme;A. Müllers;J. Walz;D. Grzonka;M. Zielinski;D. Fitzakerley;M. George;E. A. Hessels;C. H. Storry;M. Weel
通讯作者:
M. Weel
DOI:
--
发表时间:
2016
期刊:
影响因子:
--
作者:
B. Radics;Y. Yamazaki
通讯作者:
Y. Yamazaki
DOI:
--
发表时间:
2016
期刊:
影响因子:
--
作者:
A. Zubiaga;M. Ervasti;I. Makkonen;A. Harju;F. Tuomisto;M. Puska
通讯作者:
M. Puska
影响因子:
2.9
作者:
M. W. Ritter;P. Egan;V. Hughes;K. Woodle
通讯作者:
K. Woodle
影响因子:
2.9
作者:
A. Mills
通讯作者:
A. Mills