10,916 research outputs found

    The new interaction suggested by the anomalous 8^8Be transition sets a rigorous constraint on the mass range of dark matter

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    The WIMPs are considered one of the favorable dark matter (DM) candidates, but as the upper bounds on the interactions between DM and standard model (SM) particles obtained by the upgraded facilities of DM direct detections get lower and lower. Researchers turn their attentions to search for less massive DM candidates, i.e. light dark matter of MeV scale. The recently measured anomalous transition in 8^8Be suggests that there exists a vectorial boson which may mediate the interaction between DM and SM particles. Based on this scenario, we combine the relevant cosmological data to constrain the mass range of DM, and have found that there exists a model parameter space where the requirements are satisfied, a range of 10.4≲mϕ≲10.4 \lesssim m_{\phi} \lesssim 16.7 MeV for scalar DM, and 13.6≲mV≲13.6 \lesssim m_{V} \lesssim 16.7 MeV for vectorial DM is demanded. Then a possibility of directly detecting such light DM particles via the DM-electron scattering is briefly studied in this framework.Comment: 13 Pages, 7 figures, references added, version accepted by journa

    First R and I Lights and Their Photometric Analyses of GSC 02393-00680

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    We obtained complete RR and II light curves of GSC 02393-00680 in 2008 and analyzed them with the 2003 version of the W-D code. It is shown that GSC 02393-00680 is a W-type shallow contact binary system with a high mass ratio q=1.600q=1.600 and a degree of contact factor f=5.0f=5.0%(\pm1.3%). It will be a good example to check up on the TRO theory. A period investigation based on all available data suggests that the system has a small-amplitude period oscillation (A3=0.d0030A_3=0.^{d}0030; T3=1.92T_3=1.92years). This may indicate it has a moderate mass close third body, which is similar to XY Leo

    The Photometric Investigation of V921 Her using the Lunar-based Ultraviolet Telescope of Chang'e-3 mission

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    The light curve of V921 Her in ultraviolet band observed by the Lunar-based Ultraviolet Telescope (LUT) is analyzed by the Wilson-Devinney code. Our solutions conclude that V921 Her is an early type marginal contact binary system with an additional close-in component. The binary system is under poor thermal contact with a temperature difference of nearly 700K700K between the two components. The close-in component contributes about 19 %19\,\% of the total luminosity in the triple system. Combining the radial velocity study together with our photometric solutions, the mass of the primary star and secondary one are calculated to be M1=1.784(Β±0.055)MβŠ™M_1 = 1.784(\pm0.055)M_\odot, M2=0.403(Β±0.012)MβŠ™M_2 = 0.403(\pm0.012)M_\odot. The evolutionary scenario of V921 Her is discussed. All times of light minimum of V921 Her available in the bibliography are taken into account and the Oβˆ’CO - C curve is analyzed for the first time. The most probable fitting results are discussed in the paper, which also confirm the existence of a third component (P3=10.2P_3=10.2 year) around the binary system. The period of V921 Her is also undergoing a continuously rapid increase at a rate of dP/dt=+2.79Γ—10βˆ’7dayβ‹…yearβˆ’1dP/dt=+2.79\times{10^{-7}}day\cdot year^{-1}, which may due to mass transfer from the less massive component to the more massive one

    Study on radiative decays of DsJβˆ—(2860)D^*_{sJ}(2860) and Ds1βˆ—(2710)D^*_{s1}(2710) into DsD_s by means of LFQM

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    The observed resonance peak around 2.86 GeV has been carefully reexamined by the LHCb collaboration and it is found that under the peak there reside two states Ds1βˆ—(2860)D^*_{s1}(2860) and Ds3βˆ—(2860)D^*_{s3}(2860) which are considered as 13D1(csΛ‰)1^3D_1(c\bar s) and 13D3(csΛ‰)1^3D_3(c\bar s) with slightly different masses and total widths. Thus, the earlier assumption that the resonance Ds1βˆ—(2710)D^*_{s1}(2710) was a 1D1D state should not be right. We suggest to measure the partial widths of radiative decays of DsJβˆ—(2860)D^*_{sJ}(2860) and Ds1βˆ—(2710)D^*_{s1}(2710) to confirm their quantum numbers. We would consider Ds1βˆ—(2710)D^*_{s1}(2710) as 23S12^3S_1 or a pure 13D11^3D_1 state, or their mixture and respectively calculate the corresponding branching ratios as well as those of DsJβˆ—(2860)D^*_{sJ}(2860). The future precise measurement would provide us information to help identifying the structures of those resonances .Comment: 8 pages, 4 figures, 1 tabl
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