32,898 research outputs found

    The Effects of Charged Charm Mesons on the Line Shapes of the X(3872)

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    The quantum numbers J^PC = 1++ of the X(3872) and the proximity of its mass to the D*0 anti-D0 threshold imply that it is either a loosely-bound hadronic molecule whose constituents are a superposition of D*0 anti-D0 and D0 anti-D*0 or it is a virtual state of charm mesons. The line shapes of the X(3872) can discriminate between these two possibilities. At energies within a few MeV of the D*0 anti-D0 threshold, the lines shapes of the X produced in B -> K transitions are determined by its binding energy and its width. Their normalizations are determined by a short-distance constant that is different for B+ -> K+ and B0 -> K0. At energies comparable to the 8 MeV splitting between the D*0 anti-D0 and D*+ D- thresholds, the charged meson channels D*+ D- and D+ D*- have a significant effect on the line shapes of the X. We calculate the line shapes taking into account the resonant coupling between the charged and neutral 1++ channels. The line shapes and their normalizations depend on one additional scattering parameter and two additional short-distance constants associated with the B -> K transitions. The line shapes of the X resonance depend on its decay channel; they are different for J/psi pi+ pi-, J/psi pi+ pi- pi0, and D0 anti-D0 pi0. The line shapes are also different for X produced in B+ decays and in B0 decays. Some conceptual errors in previous work on this problem are pointed out.Comment: 30 pages, 7 figure

    A smartphone-based device for measuring soil organic matter

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    The project evaluated the potential of utilizing a smartphone-based system for the in-field analysis of Soil Organic Matter. Although it demonstrated that the performance of the smartphone-based spectrometer can be comparable to commercial spectrometers, the results suggest that it is challenging to identify the spectral “signatures” of the SOM due to the morphology and moisture variation of soil samples

    Weakly-bound Hadronic Molecule near a 3-body Threshold

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    The X(3872) seems to be a loosely-bound hadronic molecule whose constituents are two charm mesons. A novel feature of this molecule is that the mass difference of the constituents is close to the mass of a lighter meson that can be exchanged between them, namely the pion. We analyze this feature in a simple model with spin-0 mesons only. Various observables are calculated to next-to-leading order in the interaction strength of the exchanged meson. Renormalization requires summing a geometric series of next-to-leading order corrections. The dependence of observables on the ultraviolet cutoff can be removed by renormalizations of the mass of the heaviest meson, the coupling constant for the contact interaction between the heavy mesons, and short-distance coefficients in the operator product expansion. The next-to-leading order correction has an unphysical infrared divergence at the threshold of the two heavier mesons that can be eliminated by a further resummation that takes into account the nonzero width of the heaviest meson.Comment: 37 pages, 13 figures, submitted to Phys.Rev.

    Deuteron-like states composed of two doubly charmed baryons

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    We present a systematic investigation of the possible molecular states composed of a pair of doubly charmed baryons (ΞccΞcc\Xi_{cc}\Xi_{cc}) or one doubly charmed baryon and one doubly charmed antibaryon (ΞccΞˉcc)(\Xi_{cc}\bar{\Xi}_{cc}) within the framework of the one-boson-exchange-potential model. For the spin-triplet systems, we take into account the mixing between the 3S1{}^3S_1 and 3D1{}^3D_1 channels. For the baryon-baryon system ΞccΞcc\Xi_{cc}\Xi_{cc} with (R,I)=(3ˉ,1/2)(R,I) = (\bar{3}, 1/2) and (3ˉ,0)(\bar{3}, 0), where RR and II represent the group representation and the isospin of the system, respectively, there exist loosely bound molecular states. For the baryon-antibaryon system ΞccΞˉcc\Xi_{cc}\bar{\Xi}_{cc} with (R,I)=(8,1)(R,I) = (8, 1), (8,1/2)(8, 1/2) and (8,0)(8,0), there also exist deuteron-like molecules. The BccBˉccB_{cc}\bar{B}_{cc} molecular states may be produced at LHC. The proximity of their masses to the threshold of two doubly charmed baryons provides a clean clue to identify them.Comment: 18 pages, 8 figure

    Hadronic Molecular States Composed of Spin-323\over 2 Singly Charmed Baryons

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    We investigate the possible deuteron-like molecules composed of a pair of charmed spin-32\frac{3}{2} baryons, or one charmed baryon and one charmed antibaryon within the one-boson-exchange (OBE) model. For the spin singlet and triplet systems, we consider the couple channel effect between systems with different orbital angular momentum. Most of the systems have binding solutions. The couple channel effect plays a significant role in the formation of some loosely bound states. The possible molecular states of ΩcΩc\Omega_c^*\Omega_c^* and ΩcΩˉc\Omega_c^*\bar{\Omega}_c^* might be stable once produced.Comment: 18 pages, 7 figure
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