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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Yasunori Endo,Naohiko KinoshitaATLAS superconducting heavy-ion linac facility where a novel injection system, the RF gas cooler, allows fast reaction products to be decelerated, thermalized and bunched for rapid and efficient injection into the CPT. The CPT spectrometer and its injection system will be described in detail and its

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Yukihiro Hamasuna,Yasunori Endoed and is now independent of irregular air pressure. The temperature of the hyperboloidal precision trap is stabilized to ±0.03°C. Remaining temperature instabilities are compensated by changes in the current of a warm coil surrounding the precision trap. The frequency synthesizer is now locked to G

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Standard-Model Tests with Superallowed ,-Decay: An Important Application of Very Precise Mass Measur two standard deviations. This result can be made more definitive by experiments that require extremely precise mass measurements, in some cases on very short-lived (≤100 ms) nuclei. This talk presents the current status and future prospects for these Standard-Model tests, emphasizing the role of pr

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CODA

Recent Progress with the SMILETRAP Penning Mass Spectrometerfollowing particles and atoms have been measured with uncertainties in the region 0.3–2 ppb: p, .H, .He, .He, .Ne, .Si, .Ar, .Ge, .Se, .Kr and .Cs. It has also been shown that though we are using a warm bore the trap pressure is sufficiently low to prevent electron capture from the rest gas for exci

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Introduction to Fuzzy Information Retrieval, two standard deviations. This result can be made more definitive by experiments that require extremely precise mass measurements, in some cases on very short-lived (≤100 ms) nuclei. This talk presents the current status and future prospects for these Standard-Model tests, emphasizing the role of pr

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https://doi.org/10.1007/978-94-009-3249-4., while the molar mass of an isotope-enriched Si single crystal has so far been determined with an uncertainty of 1 · 10.. A direct comparison (for example, relative value of isotope abundances determined by (n,.)-spectrometry omitting the thermal neutron cross section) furnishes a value of 7 · 10.

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Conference proceedings 2001 (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,