2,005 research outputs found

    Weak gravity in DGP braneworld model

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    We analyze the weak gravity in the braneworld model proposed by Dvali-Gabadadze-Porrati, in which the unperturbed background spacetime is given by five dimensional Minkowski bulk with a brane which has the induced Einstein Hilbert term. This model has a critical length scale rcr_c. Naively, we expect that the four dimensional general relativity (4D GR) is approximately recovered at the scale below rcr_c. However, the simple linear perturbation does not work in this regime. Only recently the mechanism to recover 4D GR was clarified under the restriction to spherically symmetric configurations, and the leading correction to 4D GR was derived. Here, we develop an alternative formulation which can handle more general perturbations. We also generalize the model by adding bulk cosmological constant and the brane tension.Comment: 7 pages, 1 figure, references adde

    In Vitro Evaluation of an Active Heat-and-Moisture Exchanger: The Hygrovent Gold

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    BACKGROUND: To improve the heat and humidification that can be achieved with aheat-and-moisture exchanger (HME),a hybrid active (ie,adds heat and water) HME,the Hygrovent Gold,was developed. We evaluated in vitro the performance of theHygrovent Gold. METHODS: We tested the Hygrovent Gold (with and without its supplemental heat andmoisture options activated),the Hygrobac,and the Hygrovent S. We measured theabsolute humidity,using a test lung ventilated at minute volumes of 5,10,and15 L/min,in normothermic (expired temperature 34 degrees C) and hypothermic(expired temperature 28 degrees C) conditions. We also measured the HMEs' flowresistance and weight after 24 h and 48 h. RESULTS: In its active mode the Hygrovent Gold provided the highest absolutehumidity,independent of minute volume,in both normothermia and hypothermia. Therespective normothermia and hypothermia absolute humidity values at 10 L/min were36.3 + 1.3 mg/L and 27.1 + 1.0 mg/L with the active Hygrovent Gold,33.9 + 0.5mg/L and 24.2 + 0.8 mg/L with the passive Hygrovent Gold,33.8 + 0.56 mg/L and24.4 + 0.4 mg/L with the Hygrobac,and 33.9 + 0.8 mg/L and 24.6 + 0.6 mg/L withthe Hygrovent S. The efficiency of the tested HMEs did not change over time. At24 h and 48 h the increase in weight and flow resistance was highest in theactive Hygrovent Gold. CONCLUSIONS: The passive Hygrovent Gold provided adequate heat and moisture innormothermia,but the active Hygrovent Gold provided the highest humidity,inboth normothermia and hypothermia

    Intensive care of patients following orthotopic liver transplantation

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    Exotic smooth structures and symplectic forms on closed manifolds

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    We give a short proof of the (known) result that there are no Kaehler structures on exotic tori. This yields a negative solution to a problem posed by Benson and Gordon. W discuss the symplectic version of the problem and analyze results which yield an evidence for the conjecture that there are no symplectic structures on exotic tori.Comment: AMSLaTeX, 16 pages, a new version. A survey of the symplectic version of the problem is adde

    Ab initio study of ferroelectric domain walls in PbTiO3

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    We have investigated the atomistic structure of the 180-degree and 90-degree domain boundaries in the ferroelectric perovskite compound PbTiO3 using a first-principles ultrasoft-pseudopotential approach. For each case we have computed the position, thickness and creation energy of the domain walls, and an estimate of the barrier height for their motion has been obtained. We find both kinds of domain walls to be very narrow with a similar width of the order of one to two lattice constants. The energy of the 90-dergree domain wall is calculated to be 35 mJ/m^2, about a factor of four lower than the energy of its 180-degree counterpart, and only a miniscule barrier for its motion is found. As a surprising feature we detected a small offset of 0.15-0.2 eV in the electrostatic potential across the 90-degree domain wall.Comment: 12 pages, with 9 postscript figures embedded. Uses REVTEX and epsf macros. Also available at http://www.physics.rutgers.edu/~dhv/preprints/bm_dw/index.htm

    Further analysis of the quantum critical point of Ce1x_{1-x}Lax_{x}Ru2_{2}Si2_{2}

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    New data on the spin dynamics and the magnetic order of Ce1x_{1-x}Lax_{x}Ru2_{2}Si2_{2} are presented. The importance of the Kondo effect at the quantum critical point of this system is emphasized from the behaviour of the relaxation rate at high temperature and from the variation of the ordered moment with respect to the one of the N\'eel temperature for various xx.Comment: Contribution for the Festschrift on the occasion of Hilbert von Loehneysen 60 th birthday. To be published as a special issue in the Journal of Low Temperature Physic

    Orbital-selective Mott transitions: Heavy fermions and beyond

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    Quantum phase transitions in metals are often accompanied by violations of Fermi liquid behavior in the quantum critical regime. Particularly fascinating are transitions beyond the Landau-Ginzburg-Wilson concept of a local order parameter. The breakdown of the Kondo effect in heavy-fermion metals constitutes a prime example of such a transition. Here, the strongly correlated f electrons become localized and disappear from the Fermi surface, implying that the transition is equivalent to an orbital-selective Mott transition, as has been discussed for multi-band transition-metal oxides. In this article, available theoretical descriptions for orbital-selective Mott transitions will be reviewed, with an emphasis on conceptual aspects like the distinction between different low-temperature phases and the structure of the global phase diagram. Selected results for quantum critical properties will be listed as well. Finally, a brief overview is given on experiments which have been interpreted in terms of orbital-selective Mott physics.Comment: 29 pages, 4 figs, mini-review prepared for a special issue of JLT

    Golgi Outpost Synthesis Impaired by Toxic Polyglutamine Proteins Contributes to Dendritic Pathology in Neurons

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    Dendrite aberration is a common feature of neurodegenerative diseases caused by protein toxicity, but the underlying mechanisms remain largely elusive. Here, we show that nuclear polyglutamine (polyQ) toxicity resulted in defective terminal dendrite elongation accompanied by a loss of Golgi outposts (GOPs) and a decreased supply of plasma membrane (PM) in Drosophila class IV dendritic arborization (da) (C4 da) neurons. mRNA sequencing revealed that genes downregulated by polyQ proteins included many secretory pathway-related genes, including COPII genes regulating GOP synthesis. Transcription factor enrichment analysis identified CREB3L1/CrebA, which regulates COPII gene expression. CrebA overexpression in C4 da neurons restores the dysregulation of COPII genes, GOP synthesis, and PM supply. Chromatin immunoprecipitation (ChIP)-PCR revealed that CrebA expression is regulated by CREB-binding protein (CBP), which is sequestered by polyQ proteins. Furthermore, co-overexpression of CrebA and Rac1 synergistically restores the polyQ-induced dendrite pathology. Collectively, our results suggest that GOPs impaired by polyQ proteins contribute to dendrite pathology through the CBP-CrebA-COPII pathway. ? 2017 The Author(s)113Ysciescopu

    Search for B+ -> D*+ pi0 decay

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    We report on a search for the doubly Cabibbo suppressed decay B+ -> D*+ pi0, based on a data sample of 657 million BBbar pairs collected at the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric energy e+ e- collider. We find no significant signal and set an upper limit of Br(B+ -> D*+ pi0) < 3.6 x 10^-6 at the 90% confidence level. This limit can be used to constrain the ratio between suppressed and favored B -> D* pi decay amplitudes, r < 0.051, at the 90% confidence level.Comment: 5pages, 2figures, submitted to PRL (v1); PRL published version (v2: minor corrections in the text

    New agegraphic dark energy in Horava-Lifshitz cosmology

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    We investigate the new agegraphic dark energy scenario in a universe governed by Horava-Lifshitz gravity. We consider both the detailed and non-detailed balanced version of the theory, we impose an arbitrary curvature, and we allow for an interaction between the matter and dark energy sectors. Extracting the differential equation for the evolution of the dark energy density parameter and performing an expansion of the dark energy equation-of-state parameter, we calculate its present and its low-redshift value as functions of the dark energy and curvature density parameters at present, of the Horava-Lifshitz running parameter λ\lambda, of the new agegraphic dark energy parameter nn, and of the interaction coupling bb. We find that w0=0.820.08+0.08w_0=-0.82^{+0.08}_{-0.08} and w1=0.080.07+0.09w_1=0.08^{+0.09}_{-0.07}. Although this analysis indicates that the scenario can be compatible with observations, it does not enlighten the discussion about the possible conceptual and theoretical problems of Horava-Lifshitz gravity.Comment: 17 pages, no figures, version published at JCA
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