1,918,445 research outputs found

    Impurity-doping induced ferroelectricity in frustrated antiferromagnet CuFeO2

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    Dielectric responses have been investigated on the triangular-lattice antiferromagnet CuFeO2 and its site-diluted analogs CuFe1-xAlxO2 (x=0.01 and 0.02) with and without application of magnetic field. We have found a ferroelectric behavior at zero magnetic field for x=0.02. At any doping level, the onset field of the ferroelectricity always coincides with that of the noncollinear magnetic structure while the transition field dramatically decreases to zero field with Al doping. The results imply the further possibility of producing the ferroelectricity by modifying the frustrated spin structure in terms of site-doping and external magnetic field.Comment: 4 pages, 4 figure

    Coupled oscillators and Feynman's three papers

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    According to Richard Feynman, the adventure of our science of physics is a perpetual attempt to recognize that the different aspects of nature are really different aspects of the same thing. It is therefore interesting to combine some, if not all, of Feynman's papers into one. The first of his three papers is on the ``rest of the universe'' contained in his 1972 book on statistical mechanics. The second idea is Feynman's parton picture which he presented in 1969 at the Stony Brook conference on high-energy physics. The third idea is contained in the 1971 paper he published with his students, where they show that the hadronic spectra on Regge trajectories are manifestations of harmonic-oscillator degeneracies. In this report, we formulate these three ideas using the mathematics of two coupled oscillators. It is shown that the idea of entanglement is contained in his rest of the universe, and can be extended to a space-time entanglement. It is shown also that his parton model and the static quark model can be combined into one Lorentz-covariant entity. Furthermore, Einstein's special relativity, based on the Lorentz group, can also be formulated within the mathematical framework of two coupled oscillators.Comment: 31 pages, 6 figures, based on the concluding talk at the 3rd Feynman Festival (Collage Park, Maryland, U.S.A., August 2006), minor correction

    Spin gap of the three-leg S=3/2 Heisenberg tube

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    The ground-state properties of the three-leg S=3/2 Heisenberg tube are studied using the density-matrix renormalization group method. We find that the spin-excitation gap associated with a spontaneous dimerization opens for the whole coupling regime, as seen in the three-leg S=1/2 Heisenberg tube. However, in contrast to the case of S=1/2 tube, the gap increases very slowly with increasing the rung coupling and its size is only a few % or less of the leg exchange interaction in the weak- and intermediate-coupling regimes. We thus argue that, unless the rung coupling is substantially larger than the leg coupling, the gap may be quite hard to be observed experimentally. We also calcuate the quantized Berry phase to show that there exist three kinds of valence-bond-solid states depending on the ratio of leg and rung couplings.Comment: 4 pages, 5 figure

    Gauge-Higgs Unification and Quark-Lepton Phenomenology in the Warped Spacetime

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    In the dynamical gauge-Higgs unification of electroweak interactions in the Randall-Sundrum warped spacetime the Higgs boson mass is predicted in the range 120 GeV -- 290 GeV, provided that the spacetime structure is determined at the Planck scale. Couplings of quarks and leptons to gauge bosons and their Kaluza-Klein (KK) excited states are determined by the masses of quarks and leptons. All quarks and leptons other than top quarks have very small couplings to the KK excited states of gauge bosons. The universality of weak interactions is slightly broken by magnitudes of 10810^{-8}, 10610^{-6} and 10210^{-2} for μ\mu-ee, τ\tau-ee and tt-ee, respectively. Yukawa couplings become substantially smaller than those in the standard model, by a factor |\cos \onehalf \theta_W| where θW\theta_W is the non-Abelian Aharonov-Bohm phase (the Wilson line phase) associated with dynamical electroweak symmetry breaking.Comment: 34 pages, 7 eps files, comments and a reference adde

    Electromagnons in the multiferroic state of perovskite manganites with symmetric-exchange striction

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    We have investigated electrically-active magnetic excitations (electromagnons) in perovskite manganites with the EE-type (up-up-down-down) spin structure by terahertz spectroscopy. Eu1x_{1-x}Yx_xMnO3_3 (0.1x\le x\le1) and Y1y_{1-y}Luy_yMnO3_3 (0y\le y\le1) without magnetic ff-moments, which host collinear sinusoidal, AA-type, cycloidal, and EE-type spin orders, are used to examine the systematics of possible electromagnons. Three-peak structures (23, 35, 45 cm1^{-1}) of magnetic origin show up in the EE-type phase with little composition (yy) dependence of frequencies, making a contrast with the electromagnons observed in the cycloidal-spin (x0.8x\le0.8) phases. One of these electromagnon is ascribed to the zone-edge magnon mode based on the calculated magnon dispersions.Comment: 5 pages, 4 figure

    Supersymmetry at the Linear Collider

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    If supersymmetry (SUSY) is realized at the electroweak scale, its underlying structure and breaking mechanism may be explored with great precision by a future linear e+ee^+ e^- collider (LC) with a clean environment, tunable collision energy, high luminosity polarized beams, and additional eee^-e^-, eγe\gamma and γγ\gamma\gamma modes. In this report we summarize four papers submitted to the ICHEP04 conference about the precise measurements of the top squark parameters and tanβ\tan\beta, the impacts of the CP phases on the search for top/bottom squarks, the Majorana nature and CP violation in the neutralino system, the implications of the SUSY dark matter scenario for the LC experiments, and the characteristics of the neutralino sector of the next--to--minimal supersymmetric standard model at the LCComment: 5 pages, 3 figures, contribution to the proceedings of the 32nd International Conference on High-Energy Physics (ICHEP 04), Beijing, China, 16-22 Aug 200
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