ar X iv : 0 80 4 . 13 11 v 3 [ nu cl - t h ] 6 N ov 2 00 8 Neutrino masses from the “ Darmstadt oscillations ”

ar X iv : 0 80 4 . 13 11 v 4 [ nu cl - t h ] 7 N ov 2 00 8 Neutrino masses from the “ Darmstadt oscillations ”

Atominstitut der Österreichischen Universitäten, Technische Universität Wien, Wiedner Hauptstraße 8-10, A-1040 Wien, Österreich, Stefan Meyer Institut für subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, A-1090, Wien, Österreich, c Petersburg Nuclear Physics Institute, 188300 Gatchina, Orlova roscha 1, Russian Federation, Excellence Cluster Universe Technische U...

ar X iv : 0 80 4 . 13 11 v 5 [ nu cl - t h ] 2 6 M ar 2 00 9 Neutrino masses from the GSI anomaly

Atominstitut der Österreichischen Universitäten, Technische Universität Wien, Wiedner Hauptstraße 8-10, A-1040 Wien, Österreich, Stefan Meyer Institut für subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, A-1090, Wien, Österreich, c Petersburg Nuclear Physics Institute, 188300 Gatchina, Orlova roscha 1, Russian Federation, Excellence Cluster Universe Technische U...

ar X iv : h ep - p h / 02 11 13 8 v 1 1 1 N ov 2 00 2 1 Neutrino Oscillations , SUSY See - Saw Mechanism and Charged Lepton

Neutrino oscillations give clear evidence for non-vanishing neutrino masses and lepton-flavor violation (LFV) in the neutrino sector. This provides strong motivation to search for signals of LFV also in the charged lepton sector, and to probe the SUSY seesaw mechanism. We compare the sensitivity of rare radiative decays on the right-handed Majorana mass scale MR with the reach in slepton-pair p...

ar X iv : h ep - p h / 00 11 11 7 v 1 8 N ov 2 00 0 1 ( Mis ) Understanding the Atmospheric Neutrino Anomaly

ar X iv : h ep - l at / 0 01 10 13 v 3 8 N ov 2 00 0 1 Chemical potential response of meson masses at finite temperature

We study the response of meson masses to the chemical potential (∂m/∂µ) at high temperature and at zero chemical potential on N f = 2 lattice with staggered fermions. Preliminary results for the meson composed of different quarks show that ∂m/∂µ|µ=0 is negative in the confinement phase and positive in the deconfinement phase.