ar X iv : 0 71 1 . 15 67 v 1 [ he p - ph ] 1 0 N ov 2 00 7 Effect of Leptonic CP Phase in ν μ → ν μ Oscillations

ar X iv : 0 71 1 . 05 21 v 1 [ he p - ph ] 4 N ov 2 00 7 CC DIS at α 3 s in Mellin - N and Bjorken - x spaces

Third-order results for the structure functions of charged-current deep-inelastic scattering are discussed. New results for 11’th Mellin moment for F ν p−ν̄ p 2,L structure functions and 12’th moment for F ν p−ν̄ p 3 are presented as well as corresponding higher Mellin moments of differences between the respective crossing-even and -odd coefficient functions. Approximations in Bjorken-x space for...

ar X iv : n uc l - th / 0 11 20 08 v 2 1 5 Ju l 2 00 2 Theoretical Study of the 3 He ( μ − , ν μ ) 3 H Capture

ar X iv : 0 81 1 . 45 43 v 1 [ he p - ph ] 2 7 N ov 2 00 8 Aspects of the phase diagram in ( P ) NJL - like models

We discuss three applications of NJLand PNJL-like models to assess aspects of the QCD phase diagram: First, we study the effect of mesonic correlations on the pressure below and above the finite temperature phase transition within a nonlocal PNJL model beyond the mean-field approximation. Second, we reconstruct the phase boundary of an NJL model from a Taylor expansion of the chiral susceptibil...

ar X iv : 0 71 0 . 58 67 v 1 [ he p - ex ] 3 1 O ct 2 00 7 Testing the μ − e universality with K ± → l ± ν decays

The ratio RK = Γ(K± → e±ν)/Γ(K± → μ±ν) provides a very powerful probe for the weak interactions structure. This ratio of decay rates is calculated with very high precision within the Standard Model but the corrections due to the presence of New Physics could be as high as 3%. The data obtained by the NA48 experiment at the CERN SPS accelerator during a 56 hours special run in 2004 has been anal...

ar X iv : 0 80 9 . 02 63 v 1 [ he p - ph ] 1 S ep 2 00 8 CP violating phases in μ − e conversion

Experiments are planned to improve the sensitivity of μ − e conversion from the current ∼ 10 to ∼ 10 − 10. If the muon (bound to the nucleus) could be polarised, a spin asymmetry of the final state electron is sensitive to CP violating phases on lepton flavour violating operators. This is similar to extracting phases from asymmetries in the final state spin and phase space distributions of μ → ...