5,771 research outputs found

    Mass limits for the chiral color symmetry GG'-boson from LHC dijet data

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    The contributions of GG'-boson predicted by the chiral color symmetry of quarks to the differential dijet cross-sections in pppp-collisions at the LHC are calculated and analysed in dependence on two free parameters of the model, the GG' mass mGm_{G'} and mixing angle θG\theta_G. The exclusion and consistency mGθGm_{G'}-\theta_G regions imposed by the ATLAS and CMS data on dijet cross-sections are found. Using the CT10 (MSTW~2008) PDF set we show that the GG'-boson for θG=45\theta_G=45^{\circ}, i.e. the axigluon, with the masses m_{G'} < 2.3 \,\, (2.6) \,\, \mbox{TeV} and m_{G'} < 3.35 \,\, (3.25) \,\, \mbox{TeV} is excluded at the probability level of 95%95\% by the ATLAS and CMS dijet data respectively. For the other values of θG\theta_G the exclusion limits are more stringent. The mGθGm_{G'}-\theta_G regions consistent with these data at CL=68%CL=68\% and CL=90%CL=90\% are also found.Comment: 13 pages, 3 figures, accepted for publication in Modern Physics Letters

    Applications of hidden symmetries to black hole physics

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    This work is a brief review of applications of hidden symmetries to black hole physics. Symmetry is one of the most important concepts of the science. In physics and mathematics the symmetry allows one to simplify a problem, and often to make it solvable. According to the Noether theorem symmetries are responsible for conservation laws. Besides evident (explicit) spacetime symmetries, responsible for conservation of energy, momentum, and angular momentum of a system, there also exist what is called hidden symmetries, which are connected with higher order in momentum integrals of motion. A remarkable fact is that black holes in four and higher dimensions always possess a set (`tower') of explicit and hidden symmetries which make the equations of motion of particles and light completely integrable. The paper gives a general review of the recently obtained results. The main focus is on understanding why at all black holes have something (symmetry) to hide.Comment: This is an extended version of the talks at NEB-14 conference (June,Ioannina,Greece) and JGRG20 meeting (September, Kyoto, Japan

    Vacuum polarization of massive scalar fields in the spacetime of the electrically charged nonlinear black hole

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    The approximate renormalized stress-energy tensor of the quantized massive conformally coupled scalar field in the spacetime of electrically charged nonlinear black hole is constructed. It is achieved by functional differentiation of the lowest order of the DeWitt-Schwinger effective action involving coincidence limit of the Hadamard-Minakshisundaram-DeWitt-Seely coefficient a3.a_{3}. The result is compared with the analogous result derived for the Reissner-Nordstr\"om black hole. It is shown that the most important differences occur in the vicinity of the event horizon of the black hole near the extremality limit. The structure of the nonlinear black hole is briefly studied by means of the Lambert functions.Comment: 22 pages, 10 figure

    Time machines: the Principle of Self-Consistency as a consequence of the Principle of Minimal Action

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    We consider the action principle to derive the classical, non-relativistic motion of a self-interacting particle in a 4-D Lorentzian spacetime containing a wormhole and which allows the existence of closed time-like curves. For the case of a `hard-sphere' self-interaction potential we show that the only possible trajectories (for a particle with fixed initial and final positions and which traverses the wormhole once) minimizing the classical action are those which are globally self-consistent, and that the `Principle of self-consistency' (originally introduced by Novikov) is thus a natural consequence of the `Principle of minimal action.'Comment: 26 pages, plain latex; modified version includes extra constraint for collinear collision case and other minor misprints correction

    Covalently Binding the Photosystem I to Carbon Nanotubes

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    We present a chemical route to covalently couple the photosystem I (PS I) to carbon nanotubes (CNTs). Small linker molecules are used to connect the PS I to the CNTs. Hybrid systems, consisting of CNTs and the PS I, promise new photo-induced transport phenomena due to the outstanding optoelectronic properties of the robust cyanobacteria membrane protein PS I
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