A Three Dimensional Model For Direct Laser Metal Powder by Labudovic, Kovalevic

By Labudovic, Kovalevic

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Sirca, for their hospitality and partial support enabling his participation at XVIIIth European Conference on Few-Body Problems in Physics. References 1. , refs. [2,3J 2. R. Alkofer and L. von Smekal: Phys. Rept. 353, 281 (2001) 3. C. D. Roberts and S. M. Schmidt: Prog. Part. Nucl. Phys. 45, Sl (2000) 4. R. Alkofer and C. D. Roberts: Phys. Lett. B369, 101 (1996) 5. D. Kekez, B. Bistrovic and D. Klabucar: Int. J. Mod. Phys. A14, 161 (1999) 6. D. Kekez and D. Klabucar: Phys. Lett. B387, 14 (1996) 7.

1 )-(2) cannot include the effects of gluon anomaly. They give only non-anomalous contributions to qq BS solutions and masses. Fortunately, gluon anomaly is suppressed as llNc in the expansion in number of colors N c , so that the procedure of refs. [7,9,10,15]' which includes gluon anomaly only through parameterizing the anomalous shift of TJo mass, leads to very satisfactory results. For example, our TJ-TJ' mass matrix is in agreement with phenomenology and lattice results. It can be seen it leads to a very good description of TJ-TJ' mixing, although it is formulated (except in Appendix of ref.

Lett. 87, 251801 (2001) 11. K. Tsushima and D. O. Riska: Nucl. Phys. A549, 313 (1992) 12. A. Liihde and D. O. Riska: Nucl. Phys. A693, 755 (2001) 13. P. Cho and M. Wise: Phys. Rev. D49, 6228 (1994) 14. A. O. Riska: hep-phj0204230 Few-Body Systems Suppl. 14, 25-28 (2003) © sl~~s by Springer-Verlag 2003 The Chances to Produce and Detect the bbud Tetraquark at LHC D. Janc l ,*, M. Rosinal,2, D. Treleani3 , A. Del Fabbro3 1 J. Stefan Institute, 1000 Ljubljana, Slovenia 2 Faculty of Mathematics and Physics, University of Ljubljana, 1000 Ljubljana, Slovenia 3 Universita di Trieste; Dipartimento di Fisica Teorica, Strada Costiera 11, Miramare-Grignano, and'INFN, Sezione di Trieste, 1-34014 Trieste, Italy Abstract.

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