2,608 research outputs found

    B\"acklund-Darboux Transformations and Discretizations of Super KdV Equation

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    For a generalized super KdV equation, three Darboux transformations and the corresponding B\"acklund transformations are constructed. The compatibility of these Darboux transformations leads to three discrete systems and their Lax representations. The reduction of one of the B\"acklund-Darboux transformations and the corresponding discrete system are considered for Kupershmidt's super KdV equation. When all the odd variables vanish, a nonlinear superposition formula is obtained for Levi's B\"acklund transformation for the KdV equation

    A Possibility of Search for New Physics at LHCb

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    It is interesting to search for new physics beyond the standard model at LHCb. We suggest that weak decays of doubly charmed baryon such as Ξcc(3520)+,Ξcc++\Xi_{cc}(3520)^+, \Xi_{cc}^{++} to charmless final states would be a possible signal for new physics. In this work, we consider two models, i.e. the unparticle and ZZ' as examples to study such possibilities. We also discuss the cases for Ξbb0,Ξbb\Xi^0_{bb}, \Xi_{bb}^- which have not been observed yet, but one can expect to find them when LHCb begins running. Our numerical results show that these two models cannot result in sufficiently large decay widths, therefore if such modes are observed at LHCb, there must be a new physics other than the unparticle or ZZ' models.Comment: 7 pages, 3 figures, 1 table. More references and discussion adde

    The weak decays of Ξc()Ξ\Xi^{(')}_{c}\to\Xi in the light-front quark model

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    Without contamination from the final state interactions, the calculation of the branching ratios of semileptonic decays Ξc()Ξ+e+νe\Xi^{(')}_{c}\to\Xi+e^+\nu_e may provide us more information about the inner structure of charmed baryons. Moreover, by studying those processes, one can better determine the form factors of ΞcΞ\Xi_c\to\Xi which can be further applied to relevant estimates. In this work, we use the light-front quark model to carry out the computations where the three-body vertex functions for Ξc\Xi_c and Ξ\Xi are employed. To fit the new data of the Belle II, we re-adjust the model parameters and obtain βs[sq]=1.07\beta_{s[sq]}=1.07 GeV which is 2.9 times larger than βssˉ=0.366\beta_{s\bar s}=0.366 GeV. This value may imply that the ssss pair in Ξ\Xi constitutes a more compact subsystem. Furthermore, we also investigate the non-leptonic decays of Ξc()Ξ\Xi^{(')}_c\to \Xi which will be experimentally measured soon, so our model would be tested by consistency with the new data.Comment: 10 pages, 3 figures and 6 tables. arXiv admin note: text overlap with arXiv:1912.0143

    Observation of forbidden phonons and dark excitons by resonance Raman scattering in few-layer WS2_2

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    The optical properties of the two-dimensional (2D) crystals are dominated by tightly bound electron-hole pairs (excitons) and lattice vibration modes (phonons). The exciton-phonon interaction is fundamentally important to understand the optical properties of 2D materials and thus help develop emerging 2D crystal based optoelectronic devices. Here, we presented the excitonic resonant Raman scattering (RRS) spectra of few-layer WS2_2 excited by 11 lasers lines covered all of A, B and C exciton transition energies at different sample temperatures from 4 to 300 K. As a result, we are not only able to probe the forbidden phonon modes unobserved in ordinary Raman scattering, but also can determine the bright and dark state fine structures of 1s A exciton. In particular, we also observed the quantum interference between low-energy discrete phonon and exciton continuum under resonant excitation. Our works pave a way to understand the exciton-phonon coupling and many-body effects in 2D materials.Comment: 14 pages, 11 figure

    Axial Force Analysis and Roll Contour Configuration of Four-High CVC Mill

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    In order to analyze the influence of technical parameters on work roll axial force of four-high continuous variable crown (CVC) mill, the deformation analyzing model with top roll system and strip was established based on influence function method. Then a CVC work roll curve designing scheme was proposed and it was carried out on some cold rolling mill considering the requirement of comprehensive work roll axial force minimization. The status of comprehensive work roll axial force is improved considering the rolling schedule that is beneficial to the roller bearing. Corresponding to the newly designed work roll contour, the backup roll end chamfer was designed considering comprehensive performance of interroll stress concentration, comprehensive work roll axial force, and strip shape control ability. The distribution of roll wear with newly designed backup roll contour is more even according to the field application data. The newly established roll configuration scheme is beneficial to four-high CVC mill
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