PPT-Spectroscopy of S=-1 hyperon resonances with

antikaon induced mesonproduction reactions Hiroyuki Kamano KEK SeminarJAEA December 12th 2016 Outline 1 Results from spectroscopic study of Y resonances based on Dynamical CoupledChannels DCC . Photonic and Plasmonic Resonance Devices. Jae Woong Yoon. , . Kyu. Jin Lee, . Manoj. . Niraula. , Mohammad . Shyiq. . Amin. ,. and Robert Magnusson. Dept. of Electrical Engineering, University of Texas – Arlington, TX 76019, United States. Paradigm change. Mikhail . Bashkanov. University of Edinburgh. UK Nuclear Physics Summer School. II. Naïve quark model. N* puzzle. Molecular states. Exotics. Tetraquarks. Pentaquarks. Hexaquarks. Hybrids. Resonances. I. Orbital Resonances. A. Definition: An orbital resonance occurs when two orbiting bodies exert a _______ and ________ gravitational influence on each other. This usually means that their orbital periods (i.e. the time it takes to make one orbit) are related by a ratio of two _____________.. Resonances. I. Orbital Resonances. A. . Definition. : An orbital resonance occurs when two orbiting bodies exert a _______ and ________ gravitational influence on each other. This usually means that their orbital periods (i.e. the time it takes to make one orbit) are related by a ratio of two _____________.. resonances. from . magnetic-dipole lines. Yuri Ralchenko. National Institute of. Standards and Technology. Gaithersburg, MD, USA. ADAS Workshop, 2013. Supported in part by the Office of Fusion Energy Sciences, U.S. DoE. Fall . 2017. First Order Spectra. For a spectrum to be 1. st. order, the . D. n. between the chemical shifts of any given pair of nuclei must be much larger than the value of the coupling constant . Oton Vázquez Doce. Excellence Cluster Universe, TU-Munich. November . 6. , 2014. Catania, Resonance Workshop.. Oton Vazquez Doce. Strangeness in medium with KLOE. 2. The DA. F. NE collider. e. e- beams at . Differential cross sections and polarization observables from K* Photoproduction and the Search for New N* States K. Hicks, Ohio Univesity CLAS Collaboration Meeting Nov. 4, 2016 Outline Introduction: missing N* states Piet Van Duppen. ISOLDE CERN, Switzerland. IKS-. K.U.Leuven. , Belgium. K.U. Leuven. University of Western Scotland, U.K. - . K.U.Leuven. , Belgium - SCK-CEN-Mol, Belgium - . U.Gent. , Belgium - . Commenius. in . Nuclear and Hadronic Systems. H. Lenske. Institut für Theoretische Physik, U. . Giessen. a. nd. . GSI Darmstadt. 1. Agenda. :. . Interference. in open . quantum. . systems. . Continuum. . Cybern 60 121-130 1988 Springer-Verlag 1988 Oscillations A Mechanism of Feature Linking in the Visual Cortex Electrode and Correlation Analyses in the Cat Eckhorn R Bauer W Jordan M Brosch W Kruse M M 2ImImImImImIm/maxwhere ImL and ImR are the le-incident and right-incident normalized intensity distributions respectively e normalized intensity distribution naturally represents the eective cavity To 2. Nuclear Magnetic Resonance Spectroscopy. After hydrogen, the most useful atom providing information is carbon-13.. The . overall intensity of a . 13. C signal is about 6400 . times . less than the intensity of an . Marie-Laure Mauborgne. SLB. CSG17 – July 17. th. 2023. 1. Founded by a physicist and an engineer in 1926 to conduct the first geophysical measurements of rock formations . What is SLB?. (former Schlumberger).