71,320 research outputs found

    Ocyplanus megalops JACOBSON & KISTNER 1983

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    Ocyplanus megalops JACOBSON & KISTNER 1983 Ocyplanus megalops JACOBSON & KISTNER 1983: 33. M a t e r i a l:1, O. Afrika, Gomba, lux, leg. Inst. Amani (MNHUB). D i s t r i b u t i o n: Zaire, Gambia, Ivory Coast, Ghana.Published as part of Pace, R., 2012, New data and new species of Aleocharinae from Tropical Africa in the Natural History Museum of the Humboldt University, Berlin (Coleoptera, Staphylinidae), pp. 1331-1362 in Linzer biologische Beiträge 44 (2) on page 1342, DOI: 10.5281/zenodo.533529

    Proper Ferroelectricity in the Dion?Jacobson Material CsBi2Ti2NbO10: Experiment and Theory

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    A diverse range of materials and properties are exhibited by layered perovskites. We report on the synthesis, characterization, and computational investigation of a new ferroelectric?CsBi2Ti2NbO10, an n = 3 member of the Dion?Jacobson (DJ) family. Structural studies using variable temperature neutron powder diffraction indicate that a combination of octahedral rotations and polar displacements result in the polar structure. Density functional theory calculations reveal that the wider perovskite blocks in CsBi2Ti2NbO0 stabilize proper ferroelectricity, in contrast to the hybrid-improper ferroelectricity reported for all other DJ phases. Our results raise the possibility of a new class of proper ferroelectric materials analogous to the well-known Aurivillius phases

    Diurnal variation of oceanic deep cumulus convection

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    February 1976.Sponsored by NOAA National Environmental Satellite Laboratory 04-3-158-51.Observational evidence / Jacobson, R. W. -- Physical hypothesis / Gray, W. M

    Derelina nigriceps KISTNER & JACOBSON 1979

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    Derelina nigriceps KISTNER 1979 Derelina nigriceps KISTNER & JACOBSON 1979: 329. M a t e r i a l: 6 specimens, O. Afrika, Gomba, lux, leg. Inst. Amani (MNHUB). D i s t r i b u t i o n: Kenya, Tanzania, Uganda, Zaire.Published as part of Pace, R., 2012, New data and new species of Aleocharinae from Tropical Africa in the Natural History Museum of the Humboldt University, Berlin (Coleoptera, Staphylinidae), pp. 1331-1362 in Linzer biologische Beiträge 44 (2) on page 1337, DOI: 10.5281/zenodo.533529

    Direct, high-resolution measurement of furrow stiffening during division of adherent cells

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    It is unclear whether cell division is driven by cortical relaxation outside the equatorial region or cortical contractility within the developing furrow alone. To approach this question, a technique is required that can monitor spatially-resolved changes in cortical stiffness with good time resolution. We employed atomic force microscopy (AFM), in force-mapping mode, to track dynamic changes in the stiffness of the cortex of adherent cultured cells along a single scan-line during M phase, from metaphase to cytokinesis. Video microscopy, which we used to correlate the AFM data with mitotic events identified by light microscopy, indicated that the AFM force-mapping technique does not perturb dividing cells. Here we show that cortical stiffening occurs over the equatorial region about 160 seconds before any furrow appears, and that this stiffening markedly increases as the furrow starts. By contrast, polar relaxation of cells does not seem to be an obligatory event for cell division to occur

    Finite rank operators in Jacobson radical {\scr R}\sb{{\scr N}\otimes{\scr M}}

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    summary:In this paper we investigate finite rank operators in the Jacobson radical RNM\mathcal R_{\mathcal N\otimes \mathcal M} of Alg(NM)\mathop {\mathrm Alg}(\mathcal N\otimes \mathcal M), where N\mathcal N, M\mathcal M are nests. Based on the concrete characterizations of rank one operators in Alg(NM)\mathop {\mathrm Alg}(\mathcal N\otimes \mathcal M) and RNM\mathcal R_{\mathcal N\otimes \mathcal M}, we obtain that each finite rank operator in RNM\mathcal R_{\mathcal N\otimes \mathcal M} can be written as a finite sum of rank one operators in RNM\mathcal R_{\mathcal N\otimes \mathcal M} and the weak closure of RNM\mathcal R_{\mathcal N\otimes \mathcal M} equals Alg(NM)\mathop {\mathrm Alg}({\mathcal N\otimes \mathcal M}) if and only if at least one of N\mathcal N, M\mathcal M is continuous

    The Jacobson Radical and Regular Modules

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    Let A be an associative, but not necessarily commutative, ring with identity, and J = J(A) its Jacobson radical. A (unital) module is regular iff every submodule is pure (see (1)). The regular socle R(M) of a module M is the sum of all its submodules which are regular. These concepts have been introduced and studied in (2).</jats:p

    Classification of rings with toroidal Jacobson graph

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    summary:Let RR be a commutative ring with nonzero identity and J(R)J(R) the Jacobson radical of RR. The Jacobson graph of RR, denoted by JR\mathfrak J_R, is defined as the graph with vertex set RJ(R)R\setminus J(R) such that two distinct vertices xx and yy are adjacent if and only if 1xy1-xy is not a unit of RR. The genus of a simple graph GG is the smallest nonnegative integer nn such that GG can be embedded into an orientable surface SnS_n. In this paper, we investigate the genus number of the compact Riemann surface in which JR\mathfrak J_R can be embedded and explicitly determine all finite commutative rings RR (up to isomorphism) such that JR\mathfrak J_R is toroidal

    On the Jacobson radical of strongly group graded rings

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    summary:For any non-torsion group GG with identity ee, we construct a strongly GG-graded ring RR such that the Jacobson radical J(Re)J(R_e) is locally nilpotent, but J(R)J(R) is not locally nilpotent. This answers a question posed by Puczy{\l}owski

    Thermal expansion anomalies of R(Fe, M)(12) (R=Y, Nd; M=Mo and Si)

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    Structural and thermal-expansion anomaly studies on R(Fe,M)(12) (R=Nd and and Y, M=Mo and Si) compounds were performed by x-ray diffraction. Mo atoms occupy the 8i site. While Si atoms occupy the 8f and 8j sites but not the 8i site. Thermal-expansion anomaly shows only in ab plane in the Mo compounds, while becomes very weak and along with only the c axis in the Si compounds. The anomaly was attributed to the contribution of the interactions of short Fe-Fe distances similar to the previous explanation on other R-Fe intermetallics and that of other strongly positive interactions such as 8j-8j. (c) 2005 American Institute of Physics.http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000230168300025&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=8e1609b174ce4e31116a60747a720701Physics, AppliedSCI(E)EICPCI-S(ISTP)
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