5,647 research outputs found

    Symmetry energy systematics and its high density behavior

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    We explore the systematics of the density dependence of nuclear matter symmetry energy in the ambit of microscopic calculations with various energy density functionals, and find that the symmetry energy from subsaturation density to supra-saturation density can be well determined by three characteristic parameters of the symmetry energy at saturation density ρ0\rho_0 , i.e., the magnitude Esym(ρ0)E_{\text{sym}}({\rho_0 }), the density slope LL and the density curvature KsymK_{\text{sym}}. This finding opens a new window to constrain the supra-saturation density behavior of the symmetry energy from its (sub-)saturation density behavior. In particular, we obtain L=46.7Β±12.8L=46.7 \pm 12.8 MeV and Ksym=βˆ’166.9Β±168.3K_{\text{sym}}=-166.9 \pm 168.3 MeV as well as Esym(2ρ0)β‰ˆ40.2Β±12.8E_{\text{sym}}({2\rho _{0}}) \approx 40.2 \pm 12.8 MeV and L(2ρ0)β‰ˆ8.9Β±108.7L({2\rho _{0}}) \approx 8.9 \pm 108.7 MeV based on the present knowledge of Esym(ρ0)=32.5Β±0.5E_{\text{sym}}({\rho_{0}}) = 32.5 \pm 0.5 MeV, Esym(ρc)=26.65Β±0.2E_{\text{sym}}({\rho_c}) = 26.65 \pm 0.2 MeV and L(ρc)=46.0Β±4.5L({\rho_c}) = 46.0 \pm 4.5 MeV at ρc=0.11\rho_{\rm{c}}= 0.11 fmβˆ’3^{-3} extracted from nuclear mass and the neutron skin thickness of Sn isotopes. Our results indicate that the symmetry energy cannot be stiffer than a linear density dependence.In addition, we also discuss the quark matter symmetry energy since the deconfined quarks could be the right degree of freedom in dense matter at high baryon densities.Comment: 10 pages, 5 figures. Contribution to International Workshop on Multi facets of Eos and Clustering (IWM-EC 2014), May 6-9, 2014, Catania, Ital

    Recent progress on the determination of the symmetry Energy

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    We summarize the current status on constraining the density dependence of the symmetry energy from terrestrial laboratory measurements and astrophysical observations. While the value Esym(ρ0)E_{sym}({\rho_{0}}) and density slope LL of the symmetry energy at saturation density ρ0\rho_{0} can vary largely depending on the data or methods, all the existing constraints are essentially consistent with Esym(ρ0)=31±2E_{sym}({\rho_{0}}) = 31 \pm 2 MeV and L=50±20L = 50 \pm 20 MeV. The determination of the supra-saturation density behavior of the symmetry energy remains a big challenge.Comment: 12 pages, 2 figures. Plenary talk at 14th National Conference on Nuclear Structure in China, Huzhou, Zhejiang, 12-16 April, 201

    Empirical information on nuclear matter fourth-order symmetry energy from an extended nuclear mass formula

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    We establish a relation between the equation of state (EOS) of nuclear matter and the fourth-order symmetry energy asym,4(A)a_{\rm{sym,4}}(A) of finite nuclei in a semi-empirical nuclear mass formula by self-consistently considering the bulk, surface and Coulomb contributions to the nuclear mass. Such a relation allows us to extract information on nuclear matter fourth-order symmetry energy Esym,4(ρ0)E_{\rm{sym,4}}(\rho_0) at normal nuclear density ρ0\rho_0 from analyzing nuclear mass data. Based on the recent precise extraction of asym,4(A)a_{\rm{sym,4}}(A) via the double difference of the "experimental" symmetry energy extracted from nuclear masses, for the first time, we estimate a value of Esym,4(ρ0)=20.0±4.6E_{\rm{sym,4}}(\rho_0) = 20.0\pm4.6 MeV. Such a value of Esym,4(ρ0)E_{\rm{sym,4}}(\rho_0) is significantly larger than the predictions from mean-field models and thus suggests the importance of considering the effects of beyond the mean-field approximation in nuclear matter calculations.Comment: 7 pages, 1 figure. Presentation improved and discussions added. Accepted version to appear in PL

    Downlink MBER beamforming transmitter based on uplink MBER beamforming receiver for TDD-SDMA systems

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    The downlink minimum bit error rate (MBER) transmit beamforming is directly derived based on the uplink MBER receive beamforming for time division duplex (TDD) space-division multiple-access (SDMA) multiple-input multiple-output systems, where the base station (BS) is equipped with multiple antennas to support multiple single-antenna mobile terminals (MTs). It is shown that the relationship between multiuser detection and multiuser transmission can still be applied for the rank-deficient system where the number of users supported is more than the number of transmit antennas available at the BS, if the MBER design is adopted. The proposed MBER transmit beamforming scheme is capable of achieving good performance for rank-deficient TDD-SDMA systems with the support of low-complexity and high power-efficient MTs, and its robustness to the downlink and uplink noise or channel mismatch is verified using simulation
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