Author:
De Paolis L,Bazzi M,Bosnar D,Bragadireanu M,Cargnelli M,Carminati M,Clozza A,Deda G,Del Grande R,Dulski K,Fiorini C,Friščić I,Guaraldo C,Iliescu M,Iwasaki M,King P,Khreptak A,Levi Sandri P,Manti S,Marton J,Miliucci M,Moskal P,Napolitano F,Niedźwiecki S,Ohnishi H,Piscicchia K,Sada Y,Scordo A,Sgaramella F,Shi H,Silarski M,Sirghi D L,Sirghi F,Skurzok M,Wycech S,Spallone A,Toho K,Tüchler M,Vazquez Doce O,Yoshida C,Zmeskal J,Curceanu C
Abstract
Abstract
The nuclear E2 resonance effect occurs when an atomic de-excitation energy is closely matched by a nuclear excitation energy. It produces an attenuation of some of the atomic X-ray lines in the resonant isotope target. Investigating the nuclear E2 resonance effect in kaonic atoms, important information about kaon-nucleus strong interaction can be provided. The only
K
−
−
42
98
Mo
nuclear resonance effect was measured by G. L. Goldfrey, G- K. Lum and C. E. Wiegand at Lawrence Berkeley Laboratory, in 1975. The nuclear E2 resonance effect was observed in 25 hours of data taking, not enough to provide a conclusive result. In four kaonic Molybdenum isotopes (
42
94
Mo
,
42
96
Mo
,
42
98
Mo
and
42
100
Mo
), the nuclear E2 resonance effect is expected at the same transition, with similar energy values. The KAMEO (Kaonic Atoms Measuring nuclear resonance Effects Observables) experiment plans to study the E2 nuclear resonance effect in kaonic Molybdenum isotopes at the DAΦNE e+e− collider, during the SIDDHARTA-2 experiment. The experimental strategy consists of exposing four solid strip targets, each enriched with one Molybdenum isotope, to negatively charged kaons, using a germanium detector for X-ray transition measurements. A further exposure of a non-resonant
42
92
Mo
isotope solid strip target will be used as reference for standard non-resonant transitions.
Subject
Computer Science Applications,History,Education
Cited by
1 articles.
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