34,973 research outputs found

    Human Bipedalism, Evolved from Arboreal Locomotion of Two-arm Brachiation

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    Among all kinds of apes, only gibbons have the slim body as human. Gibbons can move in the forest by cross arm swing, what was the locomotion mode of our arboreal ancestor. Since our ancestor had much heavier body but weaker arms than gibbons, we suppose they had to move with two arm brachiation. Such mode of locomotion can account reasonably for the transition to bipedalism. Firstly, it needed our ancestor to straighten knee and hip joints and flex their lumbar spine. secondly, it evolved the feet of our ancestor with longitudinal arche. And most importantly, it made the ratio of the length of the upper limbs to that of the lower limbs unsuitable for quadruped walking.Comment: 10 pages, 4 figure

    Configuration mixing effects in neutron-rich carbon isotopes

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    Shell model calculations are done to study the structure of neutron-rich carbon isotopes. For both even-A and odd-A neutron-rich carbon isotopes, the energy levels are strongly affected by the configuration mixing of valence neutrons. The calculated energy levels in the nucleus 17^{17}C are significantly improved compared with experimental values when the model space of the three valence neutrons is enlarged from pure ν(0d5/2)3\nu(0d_{5/2})^{3} configuration to full sdsd space. We also investigate the configuration mixing effect on the B(E2)B(E2) values in even-even nuclei 16−20^{16-20}C

    Resonant parameters of the Y(4220)Y(4220)

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    The vector charmoniumlike state Y(4220)Y(4220) was reported recently in the cross sections of e+e−→ωχc0e^+e^-\to \omega \chi_{c0}, π+π−hc\pi^+\pi^-h_c, π+π−J/ψ\pi^+\pi^- J/\psi, and D0D∗−π++c.c.D^0 D^{*-}\pi^+ + c.c. measured by the BESIII experiment. A combined fit is performed to the cross sections of these four final states to extract the resonant parameters of the Y(4220)Y(4220). We determine a mass M=(4219.6±3.3±5.1)M=(4219.6\pm 3.3\pm 5.1)~MeV/c2c^2 and a total width Γ=(56.0±3.6±6.9)\Gamma=(56.0\pm 3.6\pm 6.9)~MeV for the Y(4220)Y(4220), where the first uncertainties are statistical and the second ones systematic. Assuming the Y(4220)Y(4220) decays dominantly to the above four modes and their isospin symmetric modes, we also estimate its leptonic decay width and decay branching fractions. These information is essential for the understanding of the nature of this state.Comment: 10 pages, 2 figures, 1 table, accepted for publication in Physical Review

    Determination of the relative phase in \psi' and J/\psi\ decays into baryon and antibaryon

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    With the recent measurements of psi' and J/psi decay into octet-baryon pairs, we study the relative phase between the strong and the electromagnetic amplitudes, and find a large phase by fitting the present data. The fits take into account the details of experimental effects, including energy spread and initial state radiation. We also predict some branching fractions of psi' decays and the continuum production rates at the J/psi mass based on the relative phase and absolute amplitudes obtained from the fits.Comment: 13 page

    Study of the Rho-pi Puzzle in Charmonium Decays

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    The theoretical explanations about the ``Rho-pi puzzle'' in charmonium decays are reviewed extensively, and the comparison of theoretical predications with experimental data is made whenever possible. Three methods to estimate the ratio of the branching fractions of J/psi and psi' decays are also discussed. It is pointed out that in order to understand the Rho-pi puzzle, and the dynamics of charmonium decays, systematic studies should be made in theory, phenomenology and experiment aspects.Comment: 13 page

    Multiple solutions in extracting physics information from experimental data

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    Multiple solutions exist in various experimental situations whenever the sum of several amplitudes is used to fit the experimentally measured distributions, such as the cross section, the mass spectrum, or the angular distribution. We show a few examples where multiple solutions were found, while only one solution was reported in the publications. Since there is no existing rules found in choosing any one of these solutions as the physics one, we propose a simple rule which agrees with what have been adopted in previous literatures: the solution corresponding to the minimal magnitudes of the amplitudes must be the physical solution. We suggest test this rule in the future experiments.Comment: 10 pages, 3 figure

    Experimental demonstration of a quantum router

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    The router is a key element for a network. We describe a scheme to realize genuine quantum routing of single-photon pulses based on cascading of conditional quantum gates in a Mach-Zehnder interferometer and report a proof-of-principle experiment for its demonstration using linear optics quantum gates. The polarization of the control photon routes in a coherent way the path of the signal photon while preserving the qubit state of the signal photon represented by its polarization. We demonstrate quantum nature of this router by showing entanglement generated between the initially unentangled control and signal photons, and confirm that the qubit state of the signal photon is well preserved by the router through quantum process tomography

    Possible determination of high-lying single particle components with (p,d) reactions

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    A detailed feasibility study on deducing the high-lying single-particle components (HLSPCs), which are important but used to be ignored, in the ground and low-lying excited states of even-even light nuclei is performed by analyses of (p,d)(p,d) reactions with \nuc{12}{C}, \nuc{24}{Mg}, \nuc{28}{Si}, and \nuc{40}{Ca} targets at 51.93 MeV. Coupled reaction channels (CRC) analyses have been made for (p,d)(p,d) transitions to the jj-forbidden excited states in \nuc{11}{C} (52−{\tfrac{5}{2}}^-, 4.32 MeV), \nuc{23}{Mg} (72+{\tfrac{7}{2}}^+, 2.05 MeV), \nuc{27}{Si} (72+{\tfrac{7}{2}}^+, 2.16 MeV) and \nuc{39}{Ca} (92−{\tfrac{9}{2}}^-, 3.64 MeV), including the major allowed transition components together with direct components of HLSPCs. Spectroscopic amplitudes of the HLSPCs are deduced by fitting the angular distributions of the ground and the jj-forbidden excited states simultaneously. The present analysis demonstrates for the first time that information about HLSPCs in atomic nuclei can be obtained from analysis of (p,d)(p,d) reactions.Comment: 7 pages, 5 figure

    Binding-energy independence of reduced single particle strengths derived from (p,d)(p,d) reactions

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    An overall reduction factor (ORF) is introduced for studying the quenching of single particle strengths through nucleon transfer reactions. The ORF includes contributions of all the probed bound states of the residual nucleus in a transfer reaction and permits a proper comparison with results of inclusive knockout reactions. A systematic analysis is made with 103 sets of angular distribution data of (p,d)(p,d) reactions on 21 even-even targets with atomic mass numbers from 8 to 56 using the consistent three-body model reaction methodology proposed in [J. Lee, J.A. Tostevin, B.A. Brown, et al., Phys. Rev. C 73, 044608 (2006)]. The extracted ORFs are found to be nearly independent on the nuclear isospin asymmetry, which is different from the systematics of inclusive knockout reactions but is consistent with the recent measurement of (d,t)(d,t), (d,3He)(d,3He), (p,2p)(p,2p), and (p,pn)(p,pn) reactions on nitrogen and oxygen isotopes and \textit{ab initio} calculations.Comment: 15 pages, 3 figure

    Possible Phase Separation and Transport Properties in Large Superconducting Ca0.77La0.18Fe0.90As2 Crystals

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    We synthesized large superconducting single crystal Ca0.77La0.18Fe0.90As2 ('112' type) of 2 millimeter size. Scanning electron microscopy (SEM) measurements revealed that bright and dark stripes alternately spread on the surface of crystals, indicating possible existence of intrinsic phase separation. Temperature (T) -dependent resistivity, Hall effect and magneto-resistance (MR) were measured with magnetic field (H) applied to different directions of crystal. The upper critical field (Hc2) anisotropy was estimated with a moderate value around 2.8. Positive Hall coefficient (RH) and anisotropic MR were found and showed strong T-dependent feature. Below T about 100 K, abnormal behaviors appear simultaneously in resistivity derivative, Hall coefficient and MR, which indicates that other scattering mechanisms more than conventional multiband effect may exist.Comment: This paper has been withdrawn by the author due to a crucial sign error of the Hall coefficien
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