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Titlebook: Atomic Physics at Accelerators: Mass Spectrometry; Proceedings of the A David Lunney,Georges Audi,H.-Jürgen Kluge Conference proceedings 20

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發(fā)表于 2025-3-21 20:05:12 | 只看該作者 |倒序瀏覽 |閱讀模式
期刊全稱Atomic Physics at Accelerators: Mass Spectrometry
期刊簡稱Proceedings of the A
影響因子2023David Lunney,Georges Audi,H.-Jürgen Kluge
視頻videohttp://file.papertrans.cn/165/164754/164754.mp4
圖書封面Titlebook: Atomic Physics at Accelerators: Mass Spectrometry; Proceedings of the A David Lunney,Georges Audi,H.-Jürgen Kluge Conference proceedings 20
影響因子The search for examples of proton radioactivity has resulted in the discovery of a large number of proton emitters in the region 50 < Z < 84 [1]. Many of these proton emitters and their daughters are also a-emitters, and in some cases the a-decay chain from the daughter terminates on a nuclide closer to stability whose mass excess is known. This opens up the possibility of using a-and proton-decay Q-values to determine the mass excesses of a large group of nuclei connected by particle decay. The Q-values are derived from the measured kinetic energies of the emitted protons or a-particles. Where the decay chains are not connected to nuclei with known mass excesses, proton separation energies can be measured in some cases and derived in others. For the a-decay ofthe parent nucleus (Z, A) to the daughter (Z - 2, A - 4), the energy and momentum relations used to convert between Q-value, mass (M) and mass excess (ME) are: M(4He)E", (1) M(Z - 2, A - 4)Erecoil, (2) Q", E", + Erecoi, ME(Z, A) Q", + ME(Z - 2, A - 4) + ME(4He). (3) In practice, one uses M(4He) ~ 4 and M(Z - 2, A - 4) (A - 4), so that Equation (3) becomes ME(Z, A) = E", (_A_) + ME(Z - 2, A - 4) + ME(4He). (4) A -4 Similarly,
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Ultra-Precise Mass Measurements Using the UW-PTMSermine the harmonic axial resonance. To illustrate the potential of this improved spectrometer, the four-fold improved measurement of the proton’s mass and the eight-fold improved measurement of oxygen’s atomic mass will be described.
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Effects of QED and Beyond from the Atomic Binding Energynd electron in the strong electromagnetic field of a heavy nucleus is considered. Special emphasis is also put on parity violation effects in atomic systems. For all systems possible investigations beyond precision tests of quantum electrodynamics are considered.
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發(fā)表于 2025-3-22 09:05:45 | 只看該作者
The Canadian Penning Trap Spectrometer at Argonne unique capabilities with respect to its initial physics program, concentrating on isotopes around the . = . line with particular emphasis on isotopes of interest to low-energy tests of the electroweak interaction and the rp-process, will be highlighted.
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[1]. Many of these proton emitters and their daughters are also a-emitters, and in some cases the a-decay chain from the daughter terminates on a nuclide closer to stability whose mass excess is known. This opens up the possibility of using a-and proton-decay Q-values to determine the mass excesses
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Fuzzy Mathematical Programming, accuracy and a novel type of CCD detector. The muonic X-rays lines serve as highly accurate calibration lines. The measurement has been accomplished recently. A detailed analysis of the data is on the way.
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