52,724 research outputs found

    Pion-photon and photon-pion transition form factors in light-cone formalism

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    We derive the minimal Fock-state expansions of the pion and the photon wave functions in light-cone formalism, then we calculate the pion-photon and the photon-pion transition form factors of γ∗π0→γ\gamma ^{\ast}\pi ^{0}\to \gamma and γ∗γ→π0\gamma ^{\ast}\gamma \to \pi ^{0} processes by employing these quark-antiquark wave functions of the pion and the photon. We find that our calculation for the γ∗γ→π0\gamma ^{\ast}\gamma \to \pi ^{0} transition form factor agrees with the experimental data at low and moderately high energy scale. Moreover, the physical differences and inherent connections between the transition form factors of γ∗π0→γ\gamma ^{\ast}\pi ^{0}\to \gamma and γ∗γ→π0 \gamma ^{\ast}\gamma \to \pi ^{0} have been illustrated, which indicate that these two physical processes are intrinsically related. In addition, we also discuss the π0→γγ\pi ^{0}\to \gamma \gamma form factor and the decay width Γ(π→γγ) \mathit{\Gamma}(\pi \to \gamma \gamma) at Q2=0Q^{2}=0.Comment: 20 pages, 2 figure

    Axial vector form factor of nucleons in a light-cone diquark model

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    The nucleon axial vector form factor is investigated in a light-cone quark spectator diquark model, in which Melosh rotations are applied to both the quark and vector diquark. It is found that this model gives a very good description of available experimental data and the results have very little dependence on the parameters of the model. The relation between the nucleon axial constant and the anomalous magnetic moment of nucleons is also discussed.Comment: 8 pages, Revtex4, 1 figure, version to be published in Phys. Rev.

    X-ray background and its correlation with the 21 cm signal

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    We use high resolution hydrodynamical simulations to study the contribution to the X-ray background from high-zz energetic sources, such as X-ray binaries, accreting nuclear black holes and shock heated interstellar medium. Adopting the model discussed in Eide et al. (2018), we find that these X-ray sources during the Epoch of Reionization (EoR) contribute less than a few percent of the unresolved X-ray background. The same sources contribute to less than ∼\sim2\% of the measured angular power spectrum of the fluctuations of the X-ray background. The outputs of radiative transfer simulations modeling the EoR are used to evaluate the cross-correlations of X-ray background with the 21~cm signal from neutral hydrogen. Such correlation could be used to confirm the origin of the 21 cm signal, as well as give information on the properties of the X-ray sources during the EoR. We find that the correlations are positive during the early stages of reionization when most of the hydrogen is neutral, while they become negative when the intergalactic medium gets highly ionized, with the transition from positive to negative depending on both the X-ray model and the scale under consideration. With {\tt SKA} as the reference instrument for the 21~cm experiment, the predicted S/N for such correlations is <1<1 if the corresponding X-ray survey is only able to resolve and remove X-ray sources with observed flux >10−15 erg cm−2 s−1>10^{-15}\,\rm erg\, cm^{-2} \, s^{-1}, while the cumulative S/N from l=1000l=1000 to 10410^{4} at xHI=0.5x_{\rm HI}=0.5 is ∼5\sim 5 if sources with observed flux >10−17 erg cm−2 s−1>10^{-17}\,\rm erg\, cm^{-2} \, s^{-1} are detected.Comment: 9 pages, 8 figure

    Melosh rotation: source of the proton's missing spin

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    It is shown that the observed small value of the integrated spin structure function for protons could be naturally understood within the naive quark model by considering the effect from Melosh rotation. The key to this problem lies in the fact that the deep inelastic process probes the light-cone quarks rather than the instant-form quarks, and that the spin of the proton is the sum of the Melosh rotated light-cone spin of the individual quarks rather than simply the sum of the light-cone spin of the quarks directly.Comment: 5 latex page

    PopIII signatures in the spectra of PopII/I GRBs

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    We investigate signatures of population III (PopIII) stars in the metal-enriched environment of GRBs originating from population II-I (PopII/I) stars by using abundance ratios derived from numerical simulations that follow stellar evolution and chemical enrichment. We find that at z>10z>10 more than 1010% of PopII/I GRBs explode in a medium previously enriched by PopIII stars (we refer to them as GRBII→\rightarrowIII). Although the formation of GRBII→\rightarrowIII is more frequent than that of pristine PopIII GRBs (GRBIIIs), we find that the expected GRBII→\rightarrowIII observed rate is comparable to that of GRBIIIs, due to the usually larger luminosities of these latter. GRBII→\rightarrowIII events take place preferentially in small proto-galaxies with stellar masses M⋆∼104.5−107 M⊙\rm M_\star \sim 10^{4.5} - 10^7\,\rm M_\odot, star formation rates SFR∼10−3−10−1 M⊙/yr\rm SFR \sim 10^{-3}-10^{-1}\,\rm M_\odot/yr and metallicities Z∼10−4−10−2 Z⊙Z \sim 10^{-4}-10^{-2}\,\rm Z_\odot. On the other hand, galaxies with Z<10−2.8 Z⊙Z < 10^{-2.8}\,\rm Z_\odot are dominated by metal enrichment from PopIII stars and should preferentially host GRBII→\rightarrowIII. Hence, measured GRB metal content below this limit could represent a strong evidence of enrichment by pristine stellar populations. We discuss how to discriminate PopIII metal enrichment on the basis of various abundance ratios observable in the spectra of GRBs' afterglows. By employing such analysis, we conclude that the currently known candidates at redshift z≃6z\simeq 6 -- i.e. GRB 050904 \cite[][]{2006Natur.440..184K} and GRB 130606A \cite[][]{2013arXiv1312.5631C} -- are likely not originated in environments pre-enriched by PopIII stars.Comment: 9 pages, 7 figures; MNRAS accepte

    Constraining the PopIII IMF with high-z GRBs

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    We study the possibility to detect and distinguish signatures of enrichment from PopIII stars in observations of PopII GRBs (GRBIIs) at high redshift by using numerical N-body/hydrodynamical simulations including atomic and molecular cooling, star formation and metal spreading from stellar populations with different initial mass functions (IMFs), yields and lifetimes. PopIII and PopII star formation regimes are followed simultaneously and both a top-heavy and a Salpeter-like IMF for pristine PopIII star formation are adopted. We find that the fraction of GRBIIs hosted in a medium previously enriched by PopIII stars (PopIII-dominated) is model independent. Typical abundance ratios, such as [Si/O] vs [C/O] and [Fe/C] vs [Si/C], can help to disentangle enrichment from massive and intermediate PopIII stars, while low-mass first stars are degenerate with regular PopII generations. The properties of galaxies hosting PopIII-dominated GRBIIs are not very sensitive to the particular assumption on the mass of the first stars.Comment: 9 pages, 4 figure

    Heavy quarkonium 2S states in light-front quark model

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    We study the charmonium 2S states ψ′\psi' and ηc′\eta_c', and the bottomonium 2S states Υ′\Upsilon' and ηb′\eta_b', using the light-front quark model and the 2S state wave function of harmonic oscillator as the approximation of the 2S quarkonium wave function. The decay constants, transition form factors and masses of these mesons are calculated and compared with experimental data. Predictions of quantities such as Br(ψ′→γηc′)(\psi' \to \gamma \eta_c') are made. The 2S wave function may help us learn more about the structure of these heavy quarkonia.Comment: 5 latex pages, final version for journal publicatio

    The 27-plet baryons with spin 3/2 under SU(3) symmetry

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    We investigate the spin 3/2 baryons in the 27-plet based on flavor SU(3) symmetry. For Jp=3/2+J^p=3/2^+, we find all the candidates for non-exotic members. For Jp=3/2−J^p=3/2^-, we predict a new non-exotic member Λ(1780)\Lambda(1780). Fitting the mass spectrum and calculating the widths of the members show an approximate symmetry of the 27-plet of SU(3). We find that the exotic members have relatively large widths and the Ξ(1950)\Xi(1950) has spin and parity Jp=3/2−J^p=3/2^-. The possibility of assigning the non-exotic candidates to an octet is also analyzed
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