1,069 research outputs found

    Many-body large polaron optical conductivity in SrTi1x_{1-x}Nbx_xO3_3

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    Recent experimental data on the optical conductivity of niobium doped SrTiO3_{3} are interpreted in terms of a gas of large polarons with effective coupling constant αeff2\alpha_{eff}\approx2. The {theoretical approach takes into account} many-body effects, the electron-phonon interaction with multiple LO-phonon branches, and the degeneracy and the anisotropy of the Ti t2g_{2g} conduction band. {Based on the Fr\"{o}hlich interaction, the many-body large-polaron theory} provides an interpretation for the essential characteristics, except -- interestingly -- for the unexpectedly large intensity of a peak at 130\sim130 meV, of the observed optical conductivity spectra of SrTi1x_{1-x}Nbx_{x}O3_{3} \textit{without} any adjustment of material parameters.Comment: to appear in Phys. Rev.

    Increased placental glucose transport rates in pregnant mice carrying fetuses with targeted disruption of their placental-specific Igf2 transcripts are not associated with raised circulating glucose concentrations.

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    At the beginning of the third week of pregnancy, mouse fetuses with targeted disruption of their paternally-transmitted insulin-like growth factor 2 gene placental-specific transcripts have growth-restricted placentas but normal body weights due to upregulated placental nutrient transport. We assessed whether increased placental glucose transport rates were associated with raised maternal glucose concentrations by performing intraperitoneal glucose tolerance tests (ipGTT) in pregnant mice carrying knockout pups and comparing them with mice carrying genotype-matched phenotypically wild type pups. Mean ± SD body weights of affected pups were 95 ± 8% of control values at e16 and 73 ± 7% at e18. There were no differences in areas under the maternal ipGTT curves at either e16 (mean ± SD being 99.0 ± 9.1% of control values; P = .9) or e18 (91.4 ± 13.4%; P = .3), suggesting that effects on transplacental glucose transport in these mice are not mediated through changes in maternal glucose concentrations

    A global disorder of imprinting in the human female germ line

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    Imprinted genes are expressed differently depending on whether they are carried by a chromosome of maternal or paternal origin. Correct imprinting is established by germline-specific modifications; failure of this process underlies several inherited human syndromes. All these imprinting control defects are cis-acting, disrupting establishment or maintenance of allele-specific epigenetic modifications across one contiguous segment of the genome. In contrast, we report here an inherited global imprinting defect. This recessive maternal-effect mutation disrupts the specification of imprints at multiple, non-contiguous loci, with the result that genes normally carrying a maternal methylation imprint assume a paternal epigenetic pattern on the maternal allele. The resulting conception is phenotypically indistinguishable from an androgenetic complete hydatidiform mole, in which abnormal extra-embryonic tissue proliferates while development of the embryo is absent or nearly so. This disorder offers a genetic route to the identification of trans-acting oocyte factors that mediate maternal imprint establishment

    Time evolution of the Rabi Hamiltonian from the unexcited vacuum

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    The Rabi Hamiltonian describes a single mode of electromagnetic radiation interacting with a two-level atom. Using the coupled cluster method, we investigate the time evolution of this system from an initially empty field mode and an unexcited atom. We give results for the atomic inversion and field occupation, and find that the virtual processes cause the field to be squeezed. No anti-bunching occurs.Comment: 25 pages, 8 figures, RevTe

    Development of an approximate method for quantum optical models and their pseudo-Hermicity

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    An approximate method is suggested to obtain analytical expressions for the eigenvalues and eigenfunctions of the some quantum optical models. The method is based on the Lie-type transformation of the Hamiltonians. In a particular case it is demonstrated that E×ϵE\times \epsilon Jahn-Teller Hamiltonian can easily be solved within the framework of the suggested approximation. The method presented here is conceptually simple and can easily be extended to the other quantum optical models. We also show that for a purely imaginary coupling the E×ϵE\times \epsilon Hamiltonian becomes non-Hermitian but Pσ0P\sigma _{0}-symmetric. Possible generalization of this approach is outlined.Comment: Paper prepared fo the "3rd International Workshop on Pseudo-Hermitian Hamiltonians in Quantum Physics" June 2005 Istanbul. To be published in Czechoslovak Journal of Physic

    Conductivity of CuO3_3-Chains: Disorder versus Electron-Phonon Coupling

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    The optical conductivity of the CuO3_3-chains, a subsystem of the 1-2-3 materials, is dominated by a broad peak in the mid-infrared (ω0.2\omega \approx 0.2eV), and a slowly falling high-frequency tail. The 1D tt-JJ-model is proposed as the relevant low-energy Hamiltonian describing the intrinsic electronic structure of the CuO3_3-chains. However, due to charge-spin decoupling, this model alone cannot reproduce the observed \sw. We consider two additional scattering mechanisms: (i) Disregarding the not so crucial spin degrees of freedom, the inclusion of strong potential disorder yields excellent agreement with experiment, but suffers from the unreasonable value of the disorder strength necessary for the fit. (ii) Moderately strong polaronic electron-phonon coupling to the mode involving Cu(1)-O(4) stretching, can be modeled within a 1D Holstein Hamiltonian of spinless fermions. Using a variational approximation for the phonon Hilbert space, we diagonalize the Hamiltonian exactly on finite lattices. As a result of the experimental hole density 1/2\approx 1/2, the chains can exhibit strong charge-density-wave (CDW) correlations, driven by phonon-mediated polaron-polaron interactions. In the vicinity of half filling, charge motion is identified as arising from moving domain walls, \ie defects in the CDW. Incorporating the effect of vacancy disorder by choosing open boundary conditions, good agreement with the experimental spectra is found. In particular, a high-frequency tail arises as a consequence of the polaron-polaron interactions.Comment: 42 pages, ETH-TH/93-31 (Postscript

    Polaronic optical absorption in electron-doped and hole-doped cuprates

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    Polaronic features similar to those previously observed in the photoinduced spectra of cuprates have been detected in the reflectivity spectra of chemically doped parent compounds of high-critical-temperature superconductors, both nn-type and pp-type. In Nd2_2CuO4y_{4-y} these features, whose intensities depend both on doping and temperature, include local vibrational modes in the far infrared and a broad band centered at \sim 1000 cm1^{-1}. The latter band is produced by the overtones of two (or three) local modes and is well described in terms of a small-polaron model, with a binding energy of about 500 cm1^{-1}. Most of the above infrared features are shown to survive in the metallic phase of Nd2x_{2-x}Cex_xCu04y_{4-y}, Bi2_2Sr2_2CuO6_6, and YBa2_2Cu3_3O7y_{7-y}, where they appear as extra-Drude peaks. The occurrence of polarons is attributed to local modes strongly coupled to carriers, as shown by a comparison with tunneling results.Comment: File latex, 31 p., submitted to Physical Review B. Figures may be faxed upon reques

    Infrared response of ordered polarons in layered perovskites

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    We report on the infrared absorption spectra of three oxides where charged superlattices have been recently observed in diffraction experiments. In La1.67_{1.67}Sr0.33_{0.33}NiO4_4, polaron localization is found to suppress the low-energy conductivity through the opening of a gap and to split the E2uE_{2u}-A2uA_{2u} vibrational manifold of the oxygen octahedra. Similar effects are detected in Sr1.5_{1.5}La0.5_{0.5}MnO4_4 and in La2_2NiO4+y_{4+y}, with peculiar differences related to the type of charge ordering.Comment: File latex, 11 p. + 3 Figures, to appear on Phys. Rev. B (Rapid Commun.), 1 Oct. 1996. The figures will be faxed upon request. E-mail:[email protected] Fax: +39-6-446315

    Inhibition of SIRT1 Reactivates Silenced Cancer Genes without Loss of Promoter DNA Hypermethylation

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    The class III histone deactylase (HDAC), SIRT1, has cancer relevance because it regulates lifespan in multiple organisms, down-regulates p53 function through deacetylation, and is linked to polycomb gene silencing in Drosophila. However, it has not been reported to mediate heterochromatin formation or heritable silencing for endogenous mammalian genes. Herein, we show that SIRT1 localizes to promoters of several aberrantly silenced tumor suppressor genes (TSGs) in which 5′ CpG islands are densely hypermethylated, but not to these same promoters in cell lines in which the promoters are not hypermethylated and the genes are expressed. Heretofore, only type I and II HDACs, through deactylation of lysines 9 and 14 of histone H3 (H3-K9 and H3-K14, respectively), had been tied to the above TSG silencing. However, inhibition of these enzymes alone fails to re-activate the genes unless DNA methylation is first inhibited. In contrast, inhibition of SIRT1 by pharmacologic, dominant negative, and siRNA (small interfering RNA)–mediated inhibition in breast and colon cancer cells causes increased H4-K16 and H3-K9 acetylation at endogenous promoters and gene re-expression despite full retention of promoter DNA hypermethylation. Furthermore, SIRT1 inhibition affects key phenotypic aspects of cancer cells. We thus have identified a new component of epigenetic TSG silencing that may potentially link some epigenetic changes associated with aging with those found in cancer, and provide new directions for therapeutically targeting these important genes for re-expression
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