3,020 research outputs found

    R+R2R + R^2 Gravity as R+R + Backreaction

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    Quadratic theory of gravity is a complicated constraint system. We investigate some consequences of treating quadratic terms perturbatively (higher derivative version of backreaction effects). This approach is shown to overcome some well known problems associated with higher derivative theories, i.e., the physical gravitational degree of freedom remains unchanged from those of Einstein gravity. Using such an interpretation of R+βR2R + \beta R^2 gravity, we investigate a classical and Wheeler DeWitt evolution of R+βR2R + \beta R^2 gravity for a particular sign of β\beta, corresponding to non- tachyon case. Matter is described by a phenomenological ρa(t)n\rho \propto a(t)^{-n}. It is concluded that both the Friedmann potential U(a)U(a) (a˙2+2U(a)=0 {\dot a}^2 + 2U(a) = 0 ) and the Wheeler DeWitt potential W(a)W(a) ([2a2+2W(a)]ψ(a)=0\left[-{\partial^2\over \partial a^2} + 2W(a)\right]\psi (a) =0 ) develop repulsive barriers near a0a\approx 0 for n>4n>4 (i.e., p>13ρ p > {1\over 3}\rho ). The interpretations is clear. Repulsive barrier in U(a)U(a) implies that a contracting FRW universe (k>0,k=0,k<0k>0, k=0, k<0) will bounce to an expansion phase without a total gravitational collapse. Repulsive barrier in W(a)W(a) means that a0a \approx 0 is a classically forbidden region. Therefore, probability of finding a universe with the big bang singularity (a=0a=0 ) is exponentially suppressed.Comment: Accepted for publication in Phy. Rev. D.,18 pages, 6 figures, Latex fil

    Dependence of the flux creep activation energy on current density and magnetic field for MgB2 superconductor

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    Systematic ac susceptibility measurements have been performed on a MgB2_2 bulk sample. We demonstrate that the flux creep activation energy is a nonlinear function of the current density U(j)j0.2U(j)\propto j^{-0.2}, indicating a nonlogarithmic relaxation of the current density in this material. The dependence of the activation energy on the magnetic field is determined to be a power law U(B)B1.33U(B)\propto B^{-1.33}, showing a steep decline in the activation energy with the magnetic field, which accounts for the steep drop in the critical current density with magnetic field that is observed in MgB2_2. The irreversibility field is also found to be rather low, therefore, the pinning properties of this new material will need to be enhanced for practical applications.Comment: 11 pages, 6 figures, Revtex forma

    Towards hardware acceleration of neuroevolution for multimedia processing applications on mobile devices

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    This paper addresses the problem of accelerating large artificial neural networks (ANN), whose topology and weights can evolve via the use of a genetic algorithm. The proposed digital hardware architecture is capable of processing any evolved network topology, whilst at the same time providing a good trade off between throughput, area and power consumption. The latter is vital for a longer battery life on mobile devices. The architecture uses multiple parallel arithmetic units in each processing element (PE). Memory partitioning and data caching are used to minimise the effects of PE pipeline stalling. A first order minimax polynomial approximation scheme, tuned via a genetic algorithm, is used for the activation function generator. Efficient arithmetic circuitry, which leverages modified Booth recoding, column compressors and carry save adders, is adopted throughout the design

    Probing the inter-layer exciton physics in a MoS2_2/MoSe2_2/MoS2_2 van der Waals heterostructure

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    Stacking atomic monolayers of semiconducting transition metal dichalcogenides (TMDs) has emerged as an effective way to engineer their properties. In principle, the staggered band alignment of TMD heterostructures should result in the formation of inter-layer excitons with long lifetimes and robust valley polarization. However, these features have been observed simultaneously only in MoSe2_2/WSe2_2 heterostructures. Here we report on the observation of long lived inter-layer exciton emission in a MoS2_2/MoSe2_2/MoS2_2 trilayer van der Waals heterostructure. The inter-layer nature of the observed transition is confirmed by photoluminescence spectroscopy, as well as by analyzing the temporal, excitation power and temperature dependence of the inter-layer emission peak. The observed complex photoluminescence dynamics suggests the presence of quasi-degenerate momentum-direct and momentum-indirect bandgaps. We show that circularly polarized optical pumping results in long lived valley polarization of inter-layer exciton. Intriguingly, the inter-layer exciton photoluminescence has helicity opposite to the excitation. Our results show that through a careful choice of the TMDs forming the van der Waals heterostructure it is possible to control the circular polarization of the inter-layer exciton emission.Comment: 19 pages, 3 figures. Just accepted for publication in Nano Letters (http://pubs.acs.org/doi/10.1021/acs.nanolett.7b03184

    Luminosity Functions of Lyman-Break Galaxies at z~4 and 5 in the Subaru Deep Field

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    We investigate the luminosity functions of Lyman-break galaxies (LBG) at z~4 and 5 based on the optical imaging data obtained in the Subaru Deep Field Project. Three samples of LBGs in a contiguous 875 arcmin^2 area are constructed. One consists of 3,808 LBGs at z~4 down to i'=26.85 selected with the B-R vs R-i' diagram. The other two consist of 539 and 240 LBGs at z~5 down to z'=26.05 selected with two kinds of two-color diagrams: V-i' vs i'-z' and R-i' vs i'-z'. The adopted selection criteria are proved to be fairly reliable by spectroscopic observation. We derive the luminosity functions of the LBGs at rest-frame ultraviolet wavelengths down to M_{UV}=-19.2 at z~4 and M_{UV}=-20.3 at z~5. We find clear evolution of the luminosity function over the redshift range of 0<z<6, which is accounted for by a sole change in the characteristic magnitude, M^*. The cosmic star formation rate (SFR) density at z~4 and z~5 is measured from the luminosity functions. We examine the evolution of the cosmic SFR density and its luminosity dependence over 0<z<6. The SFR density contributed from brighter galaxies is found to change more drastically with cosmic time. The contribution from brighter galaxies has a sharp peak around z=3-4, while that from fainter galaxies evolves relatively mildly with a broad peak at earlier epoch. Combining the observed SFR density with the standard Cold Dark Matter model, we compute the cosmic SFR per unit baryon mass in dark haloes, i.e., the specific SFR. The specific SFR is found to scale with redshift as (1+z)^3 up to z~4, implying that the efficiency of star formation is on average higher at higher redshift in proportion to the cooling rate within dark haloes, while this is not simply the case at z>4.Comment: 28 pages, 25 figures, accepted for publication in ApJ, a high resolution version of Figs.7,8,9 is available at http://hikari.astron.s.u-tokyo.ac.jp/~yoshida/sdflbglf

    Direct Photon Scattering by Plasmons in BiTeI

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    We use polarization resolved Raman spectroscopy to show that for 3D giant Rashba system the bulk plasmon collective mode directly couples to the Raman response even in the long wavelength q0\mathbf q \rightarrow 0 limit although the standard theory predicts that the plasmon spectral weight should scale as the square of its quasi-momentum and hence be negligibly weak in the Raman spectra. Such plasmon coupling to the Raman response at q0\mathbf q \rightarrow 0 arises for a polar system with spin-orbit coupling when the incoming photon excitation is turned to a resonance with Rashba-split intermediates states involved in the resonant Raman process. As an example, we identify special features of BiTeI's chiral band structure that enable the appearance of plasmon mode in the Raman spectrum

    Extracting inter-dot tunnel couplings between few donor quantum dots in silicon

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    The long term scaling prospects for solid-state quantum computing architectures relies heavily on the ability to simply and reliably measure and control the coherent electron interaction strength, known as the tunnel coupling, tc. Here, we describe a method to extract the tc between two quantum dots (QDs) utilising their different tunnel rates to a reservoir. We demonstrate the technique on a few donor triple QD tunnel coupled to a nearby single-electron transistor(SET)in silicon. The device was patterned using scanning tunneling microscopy-hydrogen lithography allowing for a direct measurement of the tunnel coupling for a given inter-dot distance. We extract tc = ± 5.5 1.8 GHz and tc = ± 2.2 1.3 GHz between each of the nearest-neighbour QDs which are separated by 14.5 nm and 14.0 nm, respectively. The technique allows for an accurate measurement of tc for nanoscale devices even when it is smaller than the electron temperature and is an ideal characterisation tool for multi-dot systems with a charge senso

    Energy Conditions in f(G)f(G) Modified Gravity with Non-minimal Coupling to Matter

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    In this paper we study a model of modified gravity with non-minimal coupling between a general function of the Gauss-Bonnet invariant, f(G)f(G), and matter Lagrangian from the point of view of the energy conditions. Such model has been introduced in Ref. [21] for description of early inflation and late-time cosmic acceleration. We present the suitable energy conditions for the above mentioned model and then, we use the estimated values of the Hubble, deceleration and jerk parameters to apply the obtained energy conditions to the specific class of modified Gauss-Bonnet models.Comment: 12 pages, no figur, Accepted for publication in Astrophysics and Space Scienc
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