Laszlo Feher, Institute for Particle and Nuclear Physics, Wigner RCP, HAS
The Ruijsenaars self-duality map as a mapping class symplectomorphism
Seminar Room, Kenkyu Honkan 3F
We explain that the self-duality symplectomorphism of the completely integrable compactified trigonometric Ruijsenaars-Schneider system arises from the natural action of the mapping class group on the moduli space of flat SU(n) connections on the one-holed torus. The talk is based on joint work with C. Klimcik reviewed in arXiv:1203.3300.
Andrew G. Akeroyd, University of Southampton
Phenomenology of the Higgs Triplet Model at the LHC
Meeting Room 1, Kenkyu Honkan 1F
The Higgs Triplet Model is a model of neutrino mass generation which predicts the existence of a doubly charged scalar and a singly charged scalar. Such particles could enhance the branching ratio of a neutral Higgs boson decaying to two photons, a channel which has been observed recently at the LHC. I also discuss the phenomenology of the doubly/singly charged scalars at the LHC, as well as summarise their ongoing searches.
森田辰弥, 東京大
量子系の弱い測定による弱値について
Seminar Room, Kenkyu Honkan 3F
量子系の測定において量子系の始状態と終状態を指定して定まる弱値が注目さ れている。本講演では弱値とその測定である弱測定の手法、及び実験的に有用 とされる弱値の測定値に対する増幅効果について紹介する。また量子力学の基 礎的側面から見た弱値の意味についても議論する。
Koji Tsumura
RG improvements on the CEDM via CP violating four-Fermi operators
Meeting room 1, Kenkyu honkan 1F
The electric dipole moment (EDM) is known to be a good probe of CP violation. In this talk, we focus the CP violating four-Fermi operators, which can mix with the EDM and chromo-EDM (CEDM) operators at one loop level. We show the renormalization-group equations (RGEs) for the (flavor-conserving) CP-violating interaction are derived up to the dimension six. We apply them to the models with the neutral scalar boson or the color-octet scalar boson which have CP-violating Yukawa interactions with quarks. Using the RGEs, the evaluation of the Barr-Zee diagram and the dimension five Weinberg operator is improved.
Kyohei Mukaida, Tokyo U
Boltzmann equation for non-equilibrium particles and its application to non-thermal dark matter production
Meeting room 1, Kenkyu honkan 1F
We consider a scalar field which is very weakly interacting with the thermal bath, and study thermal effects on the evolution of its number density. We use the Boltzmann equation derived from the Kadanoff-Baym equation, assuming that the degrees of freedom in the thermal bath are well described as “quasi-particles” with thermally modified dispersion relations. The obtained Boltzmann equation differs from the conventional one since the collision term is thermally modified through “quasi-particles.” Then, we apply this equation to the Freeze-In dark matter production scenario. We show that thermal effects can change the resultant dark matter abundance by ${cal O} (10-100) %$ compared to the result without taking account of thermal effects.
Corneliu Sochichiu, Sung KyunKwan U
Dirac Lattice or Down to High Energy
Meeting room 1, Kenkyu honkan 1F
I consider the conditions for the emergence of Dirac/Weyl/Majorana fermions from a (nonrelativistic) Fermi system.
Soichiro Goda, Kyoto U
Chiral condensate in nuclear matter beyond linear density using chiral Ward identity
Seminar room, Kenkyu honkan 3F In low-energy Quantum ChromoDynamics, spontaneous breaking of chiral symmetry is one of the most important phenomenon because this is responsible for the generation of the constituent quark mass. We focus on partial restoration of chiral symmetry in a finite density environment such as inside of atomic nucleus. Partial restoration of chiral symmetry can be observed by investigating the modification of hadron properties in nuclear matter. To examine partial restoration of chiral symmetry in nucleus experimentally, binding energy and width of 1s state of deeply bound pionic atom are measured precisely [1]. This experiment suggests that the chiral condensate which is an order parameter of the chiral symmetry breaking is reduced by about 30 % at the nuclear density. In our work [2], we analyze density corrections of the chiral condensate up to Next to leading order (NLO) using the chiral Ward identity [3] and in-medium chiral perturbation theory [4,5]. The in-medium chiral condensate is calculated by a correlation function of the axial current and pseudoscalar density in nuclear matter as a consequence of the chiral Ward identity. The correlation function is evaluated using in-medium chiral perturbation theory with the hadronic quantities of pion and nucleon dynamics. We assume that all of the in-vacuum interaction vertices are known and in-vacuum loop corrections are supposed to be done by using the experimental values of the couplings in the calculation of the condensate. This procedure leads to a density (fermi momentum) expansion. Based on this density expansion approach, we analyze diagrammatic structure of the current Green function which gives density effects to the condensate. This analysis shows that medium effects to the chiral condensate beyond linear density come from interactions between pions and nuclear matter such as pion-exchange process. As a result, we find that NLO contribution is small.
In low-energy Quantum ChromoDynamics, spontaneous breaking of chiral symmetry is one of the most important phenomenon because this is responsible for the generation of the constituent quark mass. We focus on partial restoration of chiral symmetry in a finite density environment such as inside of atomic nucleus. Partial restoration of chiral symmetry can be observed by investigating the modification of hadron properties in nuclear matter. To examine partial restoration of chiral symmetry in nucleus experimentally, binding energy and width of 1s state of deeply bound pionic atom are measured precisely [1]. This experiment suggests that the chiral condensate which is an order parameter of the chiral symmetry breaking is reduced by about 30 % at the nuclear density. In our work [2], we analyze density corrections of the chiral condensate up to Next to leading order (NLO) using the chiral Ward identity [3] and in-medium chiral perturbation theory [4,5]. The in-medium chiral condensate is calculated by a correlation function of the axial current and pseudoscalar density in nuclear matter as a consequence of the chiral Ward identity. The correlation function is evaluated using in-medium chiral perturbation theory with the hadronic quantities of pion and nucleon dynamics. We assume that all of the in-vacuum interaction vertices are known and in-vacuum loop corrections are supposed to be done by using the experimental values of the couplings in the calculation of the condensate. This procedure leads to a density (fermi momentum) expansion. Based on this density expansion approach, we analyze diagrammatic structure of the current Green function which gives density effects to the condensate. This analysis shows that medium effects to the chiral condensate beyond linear density come from interactions between pions and nuclear matter such as pion-exchange process. As a result, we find that NLO contribution is small.
[1] K. Suzuki et al., Phys. Rev. Lett. 92, 072302 (2004).
[2] S. Goda and D. Jido, in preparation. ; D. Jido, S. Goda, arXiv:1108.6144 [nucl-th].
[3] D. Jido, T. Hatsuda and T. Kunihiro, Phys. Lett. B 670,109 (2008).
[4] J. A. Oller, Phys. Rev. C 65, 025204 (2002).
[5] U. G. Meissner, J. A. Oller and A. Wirzba, Annals Phys. 297, 27(2002).
Makoto Oka, Tokyo Institute of Technology
[Particle and Nuclear Physics Seminar at J-PARC] Spectroscopy and Interaction of Heavy Hadrons
Tokai 1st building 115, KEK Tokai campus
I discuss topics on the heavy-baryon spectroscopy and its implication to QCD. I also look for possibilities of finding charmed hypernuclei.
Tatsuo Kobayashi, Kyoto
TeV scale mirage mediation in NMSSM
Meeting room 1, Kenkyu honkan 1F
We study the next-to-minimal supersymmetric standard model. We consider soft supersymmetry breaking parameters, which are induced by the mirage mediation mechanism. We concentrate on the mirage mediation, where the so-called mirage scale is the TeV scale. In this scenario, we can realize the up-type Higgs soft mass of O(200) GeV, while other masses like gaugino and stop masses are heavy such as 1 TeV. Cancellation between the effective mu-term and the down-type Higgs soft mass ameliorates the fine-tuning in the electroweak symmetry breaking. The lightest Higgs mass can be 115-130 GeV. The higgsino and singlino are light and their linear combination is the lightest superparticle.
Toru Fuda, Hokkaido U
連続的な観測を受ける量子系の数学的研究
Seminar room, Kenkyu honkan 3F
