239 research outputs found

    Chiral anomaly and strange-nonstrange mixing

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    As a first step, a simple and pedagogical recall of the η\eta-η′\eta' system is presented, in which the role of the axial anomaly, related to the heterochiral nature of the multiplet of (pseudo)scalar states, is underlined. As a consequence, η\eta is close to the octet and η′\eta' to the singlet configuration. On the contrary, for vector and tensor states, which belong to homochiral multiplets, no anomalous contribution to masses and mixing is present. Then, the isoscalar physical states are to a very good approximation nonstrange and strange, respectively. Finally, for pseudotensor states, which are part of an heterochiral multiplet (just as pseudoscalar ones), a sizable anomalous term is expected: η2(1645)\eta_2 (1645) roughly corresponds to the octet and η2(1870)\eta_2 (1870) to the singlet.Comment: 4 pages. Prepared for the proceedings of MESON 2018, 15th International Workshop on Meson Physics, KRAK\'OW, POLAND, 7th - 12th June 201

    Modelling glueballs

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    Glueballs are predicted in various theoretical approaches of QCD (most notably lattice QCD), but their experimental verification is still missing. In the low-energy sector some promising candidate for the scalar glueball exist, and some (less clear) candidates for the tensor and pseudoscalar glueballs were also proposed. Yet, for heavier gluonic states there is much work to be done both from the experimental and theoretical points of view. In these proceedings, we briefly review the current status of research of glueballs and discuss future developments.Comment: Proceedings of MESON2016, 14th International Workshop on Meson Production, Properties and Interaction KRAK\'OW, POLAND, 2-7/6/2016. 6 page

    On unitary evolution and collapse in Quantum Mechanics

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    In the framework of an interference setup in which only two outcomes are possible (such as in the case of a Mach-Zehnder interferometer), we discuss in a simple and pedagogical way the difference between a standard, unitary quantum mechanical evolution and the existence of a real collapse of the wave function. Moreover, we also present the Elitzur-Vaidman bomb, the delayed choice experiment, and the effect of decoherence. In the end, we propose two simple experiments to visualize decoherence and to test the role of an entagled particle.Comment: 24 pages, 7 figure

    Revisiting the axial anomaly for light mesons and baryons

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    The axial anomaly is responsible for the masses and mixing of the mesons η\eta and η′\eta'. An open question is if (and to what extent) it affects also other hadrons. We show that anomalous terms can be important to understand the spectroscopy of the pseudotensor mesons η2(1645)\eta_2 (1645) and η2(1870)\eta_2 (1870). In fact, pseudotensor mesons belong to a so-called heterochiral multiplet, for which a quadratic mixing term between nonstrange and strange isoscalar members arises. On the contrary, for so-called homochiral multiplets, such as the ground-state (axial-)vector and tensor mesons, this mixing is not possible, hence one can easily understand why the isoscalar members of these multiplets are almost purely nonstrange and strange, respectively. Moreover, the axial anomaly can be also coupled to baryons (within the mirror assignment), and thus it helps to explain the large decay width N∗(1535)→Nη N^{\ast }(1535)\rightarrow N\eta and to clarify which baryons are chiral partners.Comment: 6 pages. Prepared for the proceedings of the XVII International Conference on Hadron Spectroscopy and Structure - Hadron2017, 25-29 September, 2017, University of Salamanca, Salamanca, Spai
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