444,624 research outputs found

    The Large-scale ISM of SS433/W50 Revisited

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    With new high-resolution CO and HI data, we revisited the large-scale interstellar medium (ISM) environment toward the SS 433/W50 system. We find that two interesting molecular cloud (MC) concentrations, G39.315-1.155 and G40.331-4.302, are well aligned along the precession cone of SS 433 within a smaller opening angle of ~7deg. The kinematic features of the two MCs at ~73--84 km/s, as well as those of the corresponding atomic-gas counterparts, are consistent with the kinematic characteristics of SS 433. That is, the receding gas from SS 433 jet is probably responsible for the redshifted feature of G39.315-1.155 near the Galactic plane and the approaching one may power the blueshifted gas of G40.331-4.302 toward the observer. Moreover, the HI emission at VLSR~70--90 km/s displays the morphological resemblance with the radio nebula W50. We suggest that the VLSR=77\pm5 km/s gas is physically associated with SS 433/W50, leading to a near kinematic distance of 4.9\pm0.4 kpc for the system. The observed gas features, which are located outside the current radio boundaries of W50, are probably the fossil record of jet-ISM interactions at ~10^5 years ago. The energetic jets of the unique microquasar have profound effects on its ISM environment, which may facilitate the formation of molecular gas on the timescale of <0.1 Myr for the ram pressure of ~2x10^6 K cm-3.Comment: 1 table, 13 figures, to appear in the ApJ. Comments welcom

    Full quantum treatment of Rabi oscillation driven by a pulse train and its application in ion-trap quantum computation

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    Rabi oscillation of a two-level system driven by a pulse train is a basic process involved in quantum computation. We present a full quantum treatment of this process and show that the population inversion of this process collapses exponentially, has no revival phenomenon, and has a dual-pulse structure in every period. As an application, we investigate the properties of this process in ion-trap quantum computation. We find that in the Cirac--Zoller computation scheme, when the wavelength of the driving field is of the order 10βˆ’610^{-6} m, the lower bound of failure probability is of the order 10βˆ’210^{-2} after about 10210^2 controlled-NOT gates. This value is approximately equal to the generally-accepted threshold in fault-tolerant quantum computation.Comment: 22 pages, 5 figur

    Universal Correlation between Critical Temperature of Superconductivity and band structure features

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    The critical temperature (Tc{T}_\text{c}) of superconductors varies a lot. The factors governing the Tc{T}_\text{c} may hold key clues to understand the nature of the superconductivity. Thereby, Tc{T}_\text{c}-involved correlations, such as Matthias laws, Uemura law, and cuprates doping phase diagrams, have been of great concern. However, the electronic interaction being responsible for the carriers pairing in high-Tc{T}_\text{c} superconductors is still not clear, which calls for more comprehensive analyses of the experimental data in history. In this work, we propose a novel perspective for searching material gene parameters and Tc{T}_\text{c}-involved correlations. By exploring holistic band structure features of diverse superconductors, we found a universal correlation between the Tc{T}_\text{c} maxima and the electron energy levels for all kinds of superconducting materials. It suggests that the Tc{T}_\text{c} maxima are determined by the energy level of secondary-outer orbitals, rather than the band structure nearby the Fermi level. The energy level of secondary-outer orbitals is a parameter corresponding to the ratio of atomic orbital hybridization, implying that the fluctuation of the orbital hybridization is another candidate of pairing glue

    Perturbed Hankel determinant, correlation functions and Painlev\'e equations

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    We continue with the study of the Hankel determinant, Dn(t,Ξ±,Ξ²):=det⁑(∫01xj+kw(x;t,Ξ±,Ξ²)dx)j,k=0nβˆ’1, D_{n}(t,\alpha,\beta):=\det\left(\int_{0}^{1}x^{j+k}w(x;t,\alpha,\beta)dx\right)_{j,k=0}^{n-1}, generated by a Pollaczek-Jacobi type weight, w(x;t,Ξ±,Ξ²):=xΞ±(1βˆ’x)Ξ²eβˆ’t/x,x∈[0,1],Ξ±>0,Ξ²>0,tβ‰₯0. w(x;t,\alpha,\beta):=x^{\alpha}(1-x)^{\beta}{\rm e}^{-t/x}, \quad x\in [0,1], \quad \alpha>0, \quad \beta>0, \quad t\geq 0. This reduces to the "pure" Jacobi weight at t=0.t=0. We may take α∈R\alpha\in \mathbb{R}, in the situation while tt is strictly greater than 0.0. It was shown in Chen and Dai (2010), that the logarithmic derivative of this Hankel determinant satisfies a Jimbo-Miwa-Okamoto Οƒ\sigma-form of Painlev\'e \uppercase\expandafter{\romannumeral5} ({\rm P_{\uppercase\expandafter{\romannumeral5}}}). In fact the logarithmic of the Hankel determinant has an integral representation in terms of a particular {\rm P_{\uppercase\expandafter{\romannumeral5}}}. \\ In this paper, we show that, under a double scaling, where nn the dimension of the Hankel matrix tends to ∞\infty, and tt tends to 0+,0^{+}, such that s:=2n2ts:=2n^2t is finite, the double scaled Hankel determinant (effectively an operator determinant) has an integral representation in terms of a particular {\rm P_{\uppercase\expandafter{\romannumeral3}'}}. Expansions of the scaled Hankel determinant for small and large ss are found. A further double scaling with Ξ±=βˆ’2n+Ξ»,\alpha=-2n+\lambda, where nβ†’βˆžn\rightarrow \infty and t,t, tends to 0+,0^{+}, such that s:=nts:=nt is finite. In this situation the scaled Hankel determinant has an integral representation in terms of a particular {\rm P_{\uppercase\expandafter{\romannumeral5}}}, %which can be degenerate to a particular {\rm P_{\uppercase\expandafter{\romannumeral3}}} and its small and large ss asymptotic expansions are also found

    Inverse Problem of Electro-seismic Conversion

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    When a porous rock is saturated with an electrolyte, electrical fields are coupled with seismic waves via the electro-seismic conversion. Pride derived the governing models, in which Maxwell equations are coupled with Biot equations through the electro-kinetic mobility parameter. The inverse problem of the linearized electro-seismic conversion consists in two step, namely the inversion of Biot equations and the inversion of Maxwell equations. We analyze the reconstruction of conductivity and electro-kinetic mobility parameter in Maxwell equations with internal measurements, while the internal measurements are provided by the results of the inversion of Biot equations. We show that knowledge of two internal data based on well-chosen boundary conditions uniquely determine these two parameters. Moreover, a Lipschitz type stability is proved based on the same sets of well-chosen boundary conditions

    Critical edge behavior in the perturbed Laguerre ensemble and the Painleve V transcendent

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    In this paper, we consider the perturbed Laguerre unitary ensemble described by the weight function of w(x,t)=(x+t)Ξ»xΞ±eβˆ’xw(x,t)=(x+t)^{\lambda}x^{\alpha}e^{-x} with xβ‰₯0,Β t>0,Β Ξ±>0,Β Ξ±+Ξ»+1>0. x\geq 0,\ t>0,\ \alpha>0,\ \alpha+\lambda+1 > 0. The Deift-Zhou nonlinear steepest descent approach is used to analyze the limit of the eigenvalue correlation kernel. It was found that under the double scaling s=4nt,s=4nt, nβ†’βˆž,n\to \infty, tβ†’0t\to 0 such that ss is positive and finite, at the hard edge, the limiting kernel can be described by the Ο†\varphi-function related to a third-order nonlinear differential equation, which is equivalent to a particular Painlev\'e V (shorted as PV_{\rm V}) transcendent via a simple transformation. Moreover, this PV_{\rm V} transcendent is equivalent to a general Painlev\'e PIII_{\rm III} transcendent. For large s,s, the PV_{\rm V} kernel reduces to the Bessel kernel JΞ±+Ξ».\mathbf{J}_{\alpha+\lambda}. For small s,s, the PV_{\rm V} kernel reduces to another Bessel kernel JΞ±.\mathbf{J}_\alpha. At the soft edge, the limiting kernel is the Airy kernel as the classical Laguerre weight.Comment: 53 page

    Revisiting Street-to-Aerial View Image Geo-localization and Orientation Estimation

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    Street-to-aerial image geo-localization, which matches a query street-view image to the GPS-tagged aerial images in a reference set, has attracted increasing attention recently. In this paper, we revisit this problem and point out the ignored issue about image alignment information. We show that the performance of a simple Siamese network is highly dependent on the alignment setting and the comparison of previous works can be unfair if they have different assumptions. Instead of focusing on the feature extraction under the alignment assumption, we show that improvements in metric learning techniques significantly boost the performance regardless of the alignment. Without leveraging the alignment information, our pipeline outperforms previous works on both panorama and cropped datasets. Furthermore, we conduct visualization to help understand the learned model and the effect of alignment information using Grad-CAM. With our discovery on the approximate rotation-invariant activation maps, we propose a novel method to estimate the orientation/alignment between a pair of cross-view images with unknown alignment information. It achieves state-of-the-art results on the CVUSA dataset.Comment: WACV 202

    Multi-modal Aggregation for Video Classification

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    In this paper, we present a solution to Large-Scale Video Classification Challenge (LSVC2017) [1] that ranked the 1st place. We focused on a variety of modalities that cover visual, motion and audio. Also, we visualized the aggregation process to better understand how each modality takes effect. Among the extracted modalities, we found Temporal-Spatial features calculated by 3D convolution quite promising that greatly improved the performance. We attained the official metric mAP 0.8741 on the testing set with the ensemble model

    Towards Randomized Testing of qq-Monomials in Multivariate Polynomials

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    Given any fixed integer qβ‰₯2q\ge 2, a qq-monomial is of the format xi1s1xi2s2...xitst\displaystyle x^{s_1}_{i_1}x^{s_2}_{i_2}...x_{i_t}^{s_t} such that 1≀sj≀qβˆ’11\le s_j \le q-1, 1≀j≀t1\le j \le t. qq-monomials are natural generalizations of multilinear monomials. Recent research on testing multilinear monomials and qq-monomails for prime qq in multivariate polynomials relies on the property that ZqZ_q is a field when qβ‰₯2q\ge 2 is prime. When q>2q>2 is not prime, it remains open whether the problem of testing qq-monomials can be solved in some compatible complexity. In this paper, we present a randomized Oβˆ—(7.15k)O^*(7.15^k) algorithm for testing qq-monomials of degree kk that are found in a multivariate polynomial that is represented by a tree-like circuit with a polynomial size, thus giving a positive, affirming answer to the above question. Our algorithm works regardless of the primality of qq and improves upon the time complexity of the previously known algorithm for testing qq-monomials for prime q>7q>7.Comment: 21 pages, 5 figures. arXiv admin note: text overlap with arXiv:1007.2675, arXiv:1007.2678, arXiv:1007.2673 by other author

    Single-use MIMO system, Painlev\'e transcendents and double scaling

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    In this paper we study a particular Painlev\'e V (denoted PV{\rm P_{V}}) that arises from Multi-Input-Multi-Output (MIMO) wireless communication systems. Such a PVP_V appears through its intimate relation with the Hankel determinant that describes the moment generating function (MGF) of the Shannon capacity. This originates through the multiplication of the Laguerre weight or the Gamma density xΞ±eβˆ’x,β€…β€Šx>0,x^{\alpha} {\rm e}^{-x},\;x> 0, for Ξ±>βˆ’1\alpha>-1 by (1+x/t)Ξ»(1+x/t)^{\lambda} with t>0t>0 a scaling parameter. Here the Ξ»\lambda parameter "generates" the Shannon capacity, see Yang Chen and Matthew McKay, IEEE Trans. IT, 58 (2012) 4594--4634. It was found that the MGF has an integral representation as a functional of y(t)y(t) and yβ€²(t)y'(t), where y(t)y(t) satisfies the "classical form" of PVP_V. In this paper, we consider the situation where n,n, the number of transmit antennas, (or the size of the random matrix), tends to infinity, and the signal-to-noise ratio (SNR) PP tends to infinity, such that s=4n2/Ps={4n^{2}}/{P} is finite. Under such double scaling the MGF, effectively an infinite determinant, has an integral representation in terms of a "lesser" PIIIP_{III}. We also consider the situations where Ξ±=k+1/2,β€…β€Šβ€…β€Šk∈N,\alpha=k+1/2,\;\;k\in \mathbb{N}, and α∈{0,1,2,… }\alpha\in\{0,1,2,\dots\} λ∈{1,2,… },\lambda\in\{1,2,\dots\}, linking the relevant quantity to a solution of the two dimensional sine-Gordon equation in radial coordinates and a certain discrete Painlev\'e-II. From the large nn asymptotic of the orthogonal polynomials, that appears naturally, we obtain the double scaled MGF for small and large ss, together with the constant term in the large ss expansion. With the aid of these, we derive a number of cumulants and find that the capacity distribution function is non-Gaussian.Comment: 30 page
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