Results 141 to 150 of about 304 (178)
Hyperons: the strange ingredients of the nuclear equation of state. [PDF]
Proc Math Phys Eng Sci, 2018 Vidaña I.
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Imaging shapes of atomic nuclei in high-energy nuclear collisions. [PDF]
NatureSTAR Collaboration.
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In situ radiochemical doping of functionalized inorganic nanoplatforms for theranostic applications: a paradigm shift in nanooncology. [PDF]
J NanobiotechnologyGhosh S, Liang Y, Cai W, Chakravarty R.
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Production of hypernuclei from antiproton capture within a relativistic transport model. [PDF]
Eur Phys J A Hadron NuclSchmidt A +3 more
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Assessment of Carrier-Free Metallacarboranes for Targeted Radiation Therapies PBFT and BNCT: Comparative Cellular Effects and Dosimetry Studies with [<i>o</i>-FESAN]<sup>-</sup> in Breast Cancer Cells. [PDF]
Pharmaceuticals (Basel)Di Maria S +13 more
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Extremely large magnetoresistance in twisted intertwined graphene spirals. [PDF]
Nat CommunZhang Y +13 more
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Il Nuovo Cimento A, 1972
A data compilation is given of 140 meson and baryon resonances. Using the principles of nuclear physics as a guide, we deduce a set of meson and baryon excitation levels (analogous to vibrational levels) and corresponding rotational bands. The excitations occur as «excitation towers» built on a set of fundamental ground states.
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A data compilation is given of 140 meson and baryon resonances. Using the principles of nuclear physics as a guide, we deduce a set of meson and baryon excitation levels (analogous to vibrational levels) and corresponding rotational bands. The excitations occur as «excitation towers» built on a set of fundamental ground states.
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1989
Strong interactions at high energy are characterized by the production of a large number of secondary particles. For example, about ten secondaries are produced in π−p collisions at 300 GeV. Of these, four are neutral on the average. Resonances, which are rather readily produced at these energies, also have a tendency to decay through many-body ...
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Strong interactions at high energy are characterized by the production of a large number of secondary particles. For example, about ten secondaries are produced in π−p collisions at 300 GeV. Of these, four are neutral on the average. Resonances, which are rather readily produced at these energies, also have a tendency to decay through many-body ...
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AIP Conference Proceedings, 2013
We report on hadron spectroscopy using the CLAS at Jefferson Lab. We present preliminary results from photoproduction experiments studying the spectroscopy of exotic mesons, cascades (Ξ's) and Dalitz decays of pseudo-scalar mesons in the largest data sample ever to be produced at photon energies of about 5 GeV.
Carlos Salgado, null CLAS Collaboration
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We report on hadron spectroscopy using the CLAS at Jefferson Lab. We present preliminary results from photoproduction experiments studying the spectroscopy of exotic mesons, cascades (Ξ's) and Dalitz decays of pseudo-scalar mesons in the largest data sample ever to be produced at photon energies of about 5 GeV.
Carlos Salgado, null CLAS Collaboration
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NEW RESULTS IN HADRON SPECTROSCOPY
International Journal of Modern Physics A, 2004Hadron spectroscopy still follows basic 1966 physics of Sakharov, Zeldovich and Nambu. Constituent quark quasiparticles with effective masses and non-abelian color gauge electric and magnetic interactions fit all masses and magnetic moments of ground state mesons and baryons containing no more than one heavy or strange or heavy quark.
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