31,020 research outputs found

    Restrictions of generalized Verma modules to symmetric pairs

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    We initiate a new line of investigation on branching problems for generalized Verma modules with respect to complex reductive symmetric pairs (g,k). Here we note that Verma modules of g may not contain any simple module when restricted to a reductive subalgebra k in general. In this article, using the geometry of K_C orbits on the generalized flag variety G_C/P_C, we give a necessary and sufficient condition on the triple (g,k, p) such that the restriction X|_k always contains simple k-modules for any g-module XX lying in the parabolic BGG category O^p attached to a parabolic subalgebra p of g. Formulas are derived for the Gelfand-Kirillov dimension of any simple k-module occurring in a simple generalized Verma module of g. We then prove that the restriction X|_k is multiplicity-free for any generic g-module X \in O if and only if (g,k) is isomorphic to a direct sum of (A_n,A_{n-1}), (B_n,D_n), or (D_{n+1},B_n). We also see that the restriction X|_k is multiplicity-free for any symmetric pair (g, k) and any parabolic subalgebra p with abelian nilradical and for any generic g-module X \in O^p. Explicit branching laws are also presented.Comment: 31 pages, To appear in Transformation Group

    Co-NMR Knight Shift of NaxCoO2 \dot yH2O Studied in Both Superconducting Regions of the Tc-nuQ3 Phase Diagram Divided by the Nonsuperconducting Phase

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    In the temperature (T)-nuQ3 phase diagram of NaxCoO2 \dot yH2O, there exist two superconducting regions of nuQ3 separated by the nonsuperconducting region, where nuQ3 is usually estimated from the peak position of the 59Co-NQR spectra of the 5/2-7/2 transition and well-approximated here as nuQ3~3nuQ,nuQ being the interaction energy between the nuclear quadrupole moment and the electric field gradient. We have carried out measurements of the 59Co-NMR Knight shift (K) for a single crystal in the higher-nuQ3 superconducting phase and found that K begins to decrease with decreasing T at Tc for both magnetic field directions parallel and perpendicular to CoO2-planes. The result indicates together with the previous ones that the superconducting pairs are in the spin-singlet state in both phases, excluding the possibility of the spin-triplet superconductivity in this phase diagram. The superconductivity of this system spreads over the wide nuQ3 regions, but is suppressed in the narrow region located at the middle point of the region possibly due to charge instability.Comment: 8 pages, 5 figures, submitted to J. Phys. Soc. Jp

    Structure of semisimple Hopf algebras of dimension p2q2p^2q^2

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    Let p,qp,q be prime numbers with p4<qp^4<q, and kk an algebraically closed field of characteristic 0. We show that semisimple Hopf algebras of dimension p2q2p^2q^2 can be constructed either from group algebras and their duals by means of extensions, or from Radford biproduct R#kG, where kGkG is the group algebra of group GG of order p2p^2, RR is a semisimple Yetter-Drinfeld Hopf algebra in kGkGYD{}^{kG}_{kG}\mathcal{YD} of dimension q2q^2. As an application, the special case that the structure of semisimple Hopf algebras of dimension 4q24q^2 is given.Comment: 11pages, to appear in Communications in Algebr

    Special functions associated to a certain fourth order differential equation

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    We develop a theory of "special functions" associated to a certain fourth order differential operator Dμ,ν\mathcal{D}_{\mu,\nu} on R\mathbb{R} depending on two parameters μ,ν\mu,\nu. For integers μ,ν≥−1\mu,\nu\geq-1 with μ+ν∈2N0\mu+\nu\in2\mathbb{N}_0 this operator extends to a self-adjoint operator on L2(R+,xμ+ν+1dx)L^2(\mathbb{R}_+,x^{\mu+\nu+1}dx) with discrete spectrum. We find a closed formula for the generating functions of the eigenfunctions, from which we derive basic properties of the eigenfunctions such as orthogonality, completeness, L2L^2-norms, integral representations and various recurrence relations. This fourth order differential operator Dμ,ν\mathcal{D}_{\mu,\nu} arises as the radial part of the Casimir action in the Schr\"odinger model of the minimal representation of the group O(p,q)O(p,q), and our "special functions" give KK-finite vectors

    High-tip-speed, low-loading transonic fan stage. Part 3: Final report

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    Tests were conducted on a high-tip-speed, low-loading transonic fan stage to determine the performance and inlet flow distortion tolerance of the design. The fan was designed for high efficiency at a moderate pressure ratio by designing the hub section to operate at minimum loss when the tip operates with an oblique shock. The design objective was an efficiency of 86 percent at a pressure ratio of 1.5, a specific flow (flow per unit annulus area) of 42 lb/sec-sq. ft (205.1 kgm/sec-m sq), and a tip speed of 1600 ft/sec (488.6 m/sec). During testing, a peak efficiency of 84 percent was achieved at design speed and design specific flow. At the design speed and pressure ratio, the flow was 4 percent greater than design, efficiency was 81 percent, and a stall margin of 24 percent was obtained. The stall line was improved with hub radial distortion but was reduced when the stage was tested with tip radial and circumferential flow distortions. Blade-to-blade values of static pressures were measured over the rotor blade tips

    Hightip-speed, low-loading transonic fan stage. Part 2: Data compilation

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    Tests were conducted on a high-tip-speed low-loading transonic fan stage to determine the performance and inlet flow distortion tolerance of the design. Test data were recorded for overall and blade element performance with both uniform and distorted inlet flows. A tabular summary of the data and a representative selection of the computer data reduction sheets are presented

    First-Principles Study of Electronic Structure in α\alpha-(BEDT-TTF)2_2I3_3 at Ambient Pressure and with Uniaxial Strain

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    Within the framework of the density functional theory, we calculate the electronic structure of α\alpha-(BEDT-TTF)2_2I3_3 at 8K and room temperature at ambient pressure and with uniaxial strain along the aa- and bb-axes. We confirm the existence of anisotropic Dirac cone dispersion near the chemical potential. We also extract the orthogonal tight-binding parameters to analyze physical properties. An investigation of the electronic structure near the chemical potential clarifies that effects of uniaxial strain along the a-axis is different from that along the b-axis. The carrier densities show T2T^2 dependence at low temperatures, which may explain the experimental findings not only qualitatively but also quantitatively.Comment: 10 pages, 7 figure
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