14,836 research outputs found

    New polynomial and multidimensional extensions of classical partition results

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    In the 1970s Deuber introduced the notion of (m,p,c)(m,p,c)-sets in N\mathbb{N} and showed that these sets are partition regular and contain all linear partition regular configurations in N\mathbb{N}. In this paper we obtain enhancements and extensions of classical results on (m,p,c)(m,p,c)-sets in two directions. First, we show, with the help of ultrafilter techniques, that Deuber's results extend to polynomial configurations in abelian groups. In particular, we obtain new partition regular polynomial configurations in Zd\mathbb{Z}^d. Second, we give two proofs of a generalization of Deuber's results to general commutative semigroups. We also obtain a polynomial version of the central sets theorem of Furstenberg, extend the theory of (m,p,c)(m,p,c)-systems of Deuber, Hindman and Lefmann and generalize a classical theorem of Rado regarding partition regularity of linear systems of equations over N\mathbb{N} to commutative semigroups.Comment: Some typos, including a terminology confusion involving the words `clique' and `shape', were fixe

    The phase diagram in the SU(3) Nambu-Jona-Lasinio model with 't Hooft and eight-quark interactions

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    It is shown that the endpoint of the first order transition line which merges into a crossover regime in the phase diagram of the Nambu--Jona-Lasinio model, extended to include the six-quark 't Hooft and eight-quark interaction Lagrangians, is pushed towards vanishing chemical potential and higher temperatures with increasing strength of the OZI-violating eight-quark interactions. We clarify a connection between the location of the endpoint in the phase diagram and the mechanism of chiral symmetry breaking at the quark level. Constraints on the coupling strengths based on groundstate stability and physical considerations are explained.Comment: 5 pages, 3 figures, prepared for the proceedings of Hadron 2009 - XIII International Conference on Hadron Spectroscopy, November 29 - December 4, Florida State University (USA

    The Polyakov-Nambu-Jona-Lasinio model with six and eight quark interactions

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    The extension of the Nambu-Jona-Lasino Model with six and eight quark interactions to include the Polyakov loop is analysed. Several interesting features are determined to be an effect of the choice of the regularization procedure. The use of a Pauli-Villars covariant regularization enables a coherent and correct description of several quantities.Comment: 3 pages, 6 figures, to appear in the conference proceedings for Quark Confinement and the Hadron Spectrum IX, August 30- September 3 2010, Madrid (Spain

    Optimal Invariant Similar Tests for Instrumental Variables Regression

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    This paper considers tests of the parameter on endogenous variables in an instrumental variables regression model. The focus is on determining tests that have certain optimal power properties. We start by considering a model with normally distributed errors and known error covariance matrix. We consider tests that are similar and satisfy a natural rotational invariance condition. We determine tests that maximize weighted average power (WAP) for arbitrary weight functions among invariant similar tests. Such tests include point optimal (PO) invariant similar tests. The results yield the power envelope for invariant similar tests. This allows one to assess and compare the power properties of existing tests, such as the Anderson-Rubin, Lagrange multiplier (LM), and conditional likelihood ratio (CLR) tests, and new optimal WAP and PO invariant similar tests. We find that the CLR test is quite close to being uniformly most powerful invariant among a class of two-sided tests. A new unconditional test, P*, also is found to have this property. For one-sided alternatives, no test achieves the invariant power envelope, but a new test. the one-sided CLR test. is found to be fairly close. The finite sample results of the paper are extended to the case of unknown error covariance matrix and possibly non-normal errors via weak instrument asymptotics. Strong instrument asymptotic results also are provided because we seek tests that perform well under both weak and
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