8,887 research outputs found

    A Novel Self-Intersection Penalty Term for Statistical Body Shape Models and Its Applications in 3D Pose Estimation

    Full text link
    Statistical body shape models are widely used in 3D pose estimation due to their low-dimensional parameters representation. However, it is difficult to avoid self-intersection between body parts accurately. Motivated by this fact, we proposed a novel self-intersection penalty term for statistical body shape models applied in 3D pose estimation. To avoid the trouble of computing self-intersection for complex surfaces like the body meshes, the gradient of our proposed self-intersection penalty term is manually derived from the perspective of geometry. First, the self-intersection penalty term is defined as the volume of the self-intersection region. To calculate the partial derivatives with respect to the coordinates of the vertices, we employed detection rays to divide vertices of statistical body shape models into different groups depending on whether the vertex is in the region of self-intersection. Second, the partial derivatives could be easily derived by the normal vectors of neighboring triangles of the vertices. Finally, this penalty term could be applied in gradient-based optimization algorithms to remove the self-intersection of triangular meshes without using any approximation. Qualitative and quantitative evaluations were conducted to demonstrate the effectiveness and generality of our proposed method compared with previous approaches. The experimental results show that our proposed penalty term can avoid self-intersection to exclude unreasonable predictions and improves the accuracy of 3D pose estimation indirectly. Further more, the proposed method could be employed universally in triangular mesh based 3D reconstruction

    Quantum Decoherence with Holography

    Get PDF
    Quantum decoherence is the loss of a system's purity due to its interaction with the surrounding environment. Via the AdS/CFT correspondence, we study how a system decoheres when its environment is a strongly-coupled theory. In the Feynman-Vernon formalism, we compute the influence functional holographically by relating it to the generating function of Schwinger-Keldysh propagators and thereby obtain the dynamics of the system's density matrix. We present two exactly solvable examples: (1) a straight string in a BTZ black hole and (2) a scalar probe in AdS5_5. We prepare an initial state that mimics Schr\"odinger's cat and identify different stages of its decoherence process using the time-scaling behaviors of R\'enyi entropy. We also relate decoherence to local quantum quenches, and by comparing the time evolution behaviors of the Wigner function and R\'enyi entropy we demonstrate that the relaxation of local quantum excitations leads to the collapse of its wave-function.Comment: 55 pages, 13 figures; v2 47 pages & 13 figs, minor revision to match published versio

    Electron Flavored Dark Matter

    Full text link
    In this paper we investigate the phenomenology of the electron flavored Dirac dark matter with two types of portal interactions. We analyze constraints from the electron magnetic moment anomaly, LHC searches of singly charged scalar, dark matter relic abundance as well as direct and indirect detections. Our study shows that the available parameter space is quite constrained, but there are parameter space that is compatible with the current data. We further show that the DAMPE cosmic ray electron excess, which indicates cosmic ray excess at around 1.5 TeV, can be interpreted as the annihilation of dark matter into electron positron pairs in this model.Comment: 6 pages, 5 figure

    Magnetic moments of the spin-32{3\over 2} doubly heavy baryons

    Full text link
    In this work, we investigate the chiral corrections to the magnetic moments of the spin-323\over 2 doubly charmed baryons systematically up to next-to-next-to-leading order with the heavy baryon chiral perturbation theory. The numerical results are given up to next-to-leading order: μΞcc∗++=1.72μN\mu_{\Xi^{*++}_{cc}}=1.72\mu_{N}, μΞcc∗+=−0.09μN\mu_{\Xi^{*+}_{cc}}=-0.09\mu_{N}, μΩcc∗+=0.99μN\mu_{\Omega^{*+}_{cc}}=0.99\mu_{N}. As a by-product, we have also calculated the magnetic moments of the spin-323\over 2 doubly bottom baryons and charmed bottom baryons: μΞbb∗0=0.63μN\mu_{\Xi^{*0}_{bb}}=0.63\mu_{N}, μΞbb∗−=−0.79μN\mu_{\Xi^{*-}_{bb}}=-0.79\mu_{N}, μΩbb∗−=0.12μN\mu_{\Omega^{*-}_{bb}}=0.12\mu_{N}, μΞbc∗+=1.12μN\mu_{\Xi^{*+}_{bc}}=1.12\mu_{N}, μΞbc∗0=−0.40μN\mu_{\Xi^{*0}_{bc}}=-0.40\mu_{N}, μΩbc∗0=0.56μN\mu_{\Omega^{*0}_{bc}}=0.56\mu_{N}.Comment: 10 pages,2 figures. arXiv admin note: text overlap with arXiv:1707.02765. Replace the published versio
    • …
    corecore