ar X iv : 0 70 8 . 32 85 v 1 [ he p - ph ] 2 4 A ug 2 00 7 Do cc̄nn̄ bound states exist ?

ar X iv : 0 80 8 . 02 85 v 1 [ he p - ph ] 3 A ug 2 00 8 Hints from Tevatron , a prelude to what ?

We comment on the recent results from the Tevatron experiments in the W+jets channel and consider some models as the possible underlying physical theories. We also list some channels for further studies.

ar X iv : 0 70 8 . 26 18 v 1 [ as tr o - ph ] 2 0 A ug 2 00 7 Using Local Volume data to constrain Dark Matter dynamics

ar X iv : 0 90 8 . 20 03 v 1 [ he p - ph ] 1 4 A ug 2 00 9 Analysis of the pseudoscalar partner of the Y ( 4660 ) and related bound states

In this article, we study the pseudoscalar bound state η c f0(980) (irrespective of the hadro-charmonium and the molecular state) with the QCD sum rules. Considering the SU(3) symmetry of the light flavor quarks and the heavy quark symmetry, we also study the bound states η cσ(400 − 1200), η b f0(980) and η b σ(400− 1200), and make reasonable predictions for their masses. PACS number: 12.39.Mk,...

ar X iv : 0 80 8 . 10 23 v 1 [ qu an t - ph ] 7 A ug 2 00 8 CATEGORICAL QUANTUM MECHANICS

ar X iv : 0 70 8 . 29 64 v 1 [ qu an t - ph ] 2 2 A ug 2 00 7 General multipartite entangled states and complex projective variety

We discuss and investigate the geometrical structure of general multipartite states. In particular, we show that a geometrical measure of entanglement for general multipartite states can be constructed by the complex projective varieties defined by quadratic polynomials.