26,119 research outputs found

    Monomial, Gorenstein and Bass Orders

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    In this article we study a class of orders called {\it monomial orders} in a central simple algebra over a non-Archimedean local field. Monomial orders are easily represented and they may be also viewed as a direct generalization of Eichler orders in quaternion algebras. A criterion for monomial orders to be Gorenstein or to be Bass is given. It is shown that a monomial order is Bass if and only if it is either a hereditary or an Eichler order of period two.Comment: 13 pages; fix typos in the proof of Theorem 3.

    Masses of Scalar and Axial-Vector B Mesons Revisited

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    The SU(3) quark model encounters a great challenge in describing even-parity mesons. Specifically, the qqΛ‰q\bar q quark model has difficulties in understanding the light scalar mesons below 1 GeV, scalar and axial-vector charmed mesons and 1+1^+ charmonium-like state X(3872)X(3872). A common wisdom for the resolution of these difficulties lies on the coupled channel effects which will distort the quark model calculations. In this work, we focus on the near mass degeneracy of scalar charmed mesons, Ds0βˆ—D_{s0}^* and D0βˆ—0D_0^{*0}, and its implications. Within the framework of heavy meson chiral perturbation theory, we show that near degeneracy can be qualitatively understood as a consequence of self-energy effects due to strong coupled channels. Quantitatively, the closeness of Ds0βˆ—D_{s0}^* and D0βˆ—0D_0^{*0} masses can be implemented by adjusting two relevant strong couplings and the renormalization scale appearing in the loop diagram. Then this in turn implies the mass similarity of Bs0βˆ—B_{s0}^* and B0βˆ—0B_0^{*0} mesons. The P0βˆ—P1β€²P_0^* P'_1 interaction with the Goldstone boson is crucial for understanding the phenomenon of near degeneracy. Based on heavy quark symmetry in conjunction with corrections from QCD and 1/mQ1/m_Q effects, we obtain the masses of B(s)0βˆ—B^*_{(s)0} and B(s)1β€²B'_{(s)1} mesons, for example, MBs0βˆ—=(5715Β±1) MeV+δΔSM_{B_{s0}^*}= (5715\pm1)\,{\rm MeV}+\delta\Delta_S, MBs1β€²=(5763Β±1) MeV+δΔSM_{B'_{s1}}=(5763\pm1)\,{\rm MeV}+\delta\Delta_S with δΔS\delta\Delta_S being 1/mQ1/m_Q corrections. We find that the predicted mass difference of 48 MeV between Bs1β€²B'_{s1} and Bs0βˆ—B_{s0}^* is larger than that of 20∼3020\sim 30 MeV inferred from the relativistic quark models, whereas the difference of 15 MeV between the central values of MBs1β€²M_{B'_{s1}} and MB1β€²M_{B'_1} is much smaller than the quark model expectation of 60βˆ’10060-100 MeV.Comment: 21 pages, 1 figure, to appear in Eur. Phys. J. (2017). arXiv admin note: text overlap with arXiv:1404.377

    Supersingular abelian surfaces and Eichler class number formula

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    Let FF be a totally real field with ring of integers OFO_F, and DD be a totally definite quaternion algebra over FF. A well-known formula established by Eichler and then extended by K\"orner computes the class number of any OFO_F-order in DD. In this paper we generalize the Eichler class number formula so that it works for arbitrary Z\mathbb{Z}-orders in DD. The motivation is to count the isomorphism classes of supersingular abelian surfaces in a simple isogeny class over a prime finite field Fp\mathbb{F}_p. We give explicit formulas for the number of these isomorphism classes for all primes pp.Comment: 29 pages, 3 numerical tables, shortened revised version with same results, Sections 7-9 of v2 are remove
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