7,678 research outputs found

    Derivation of upward muon energy spectra in the TeV range produced by neutrinos from 3C273 AGN and diffuse atmospheric sources

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    The neutrino-induced upward muon energy spectrum on Earth at the TeV energy range emitted by the point source 3C273 AGN has been calculated using the AGN-emitted neutrino spectrum of Szabo and Protheroe and the result has been compared with that expected from background neutrinos. The QCD-based model of Berezinsky et al. has been fairly employed to estimate the muon contribution due to the charge current interactions in rock. The diffuse neutrino-induced upward muon energy spectrum from AGN sources has also been estimated and compared with the expected results from the spectra of prompt neutrinos and atmospheric backgrounds. It is found that the upward muon fluxes generated by AGN neutrinos are dominating the Universe beyond 10 TeV muon energy

    Pion Production Spectrum at the Atmosphere in the Energy Range 3-100 G eV

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    μ\muSR and Neutron Diffraction Investigations on Reentrant Ferromagnetic Superconductor Eu(Fe{0.86}Ir{0.14})2As2

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    Results of muon spin relaxation (μ\muSR) and neutron powder diffraction measurements on a reentrant superconductor Eu(Fe0.86_{0.86}Ir0.14_{0.14})2_2As2_2 are presented. Eu(Fe0.86_{0.86}Ir0.14_{0.14})2_2As2_2 exhibits superconductivity at Tcon22.5T_{\rm c\,on} \approx 22.5~K competing with long range ordered Eu+2^{+2} moments below 18\approx 18 K. A reentrant behavior (manifested by nonzero resistivity in the temperature range 10--17.5 K) results from an exquisite competition between the superconductivity and magnetic order. The zero field μ\muSR data confirm the long range magnetic ordering below TEu=18.7(2)T_{\rm Eu} = 18.7(2) K. The transition temperature is found to increase with increasing magnetic field in longitudinal field μ\muSR which along with the neutron diffraction results, suggests the transition to be ferromagnetic. The neutron diffraction data reveal a clear presence of magnetic Bragg peaks below TEuT_{\rm Eu} which could be indexed with propagation vector k = (0, 0, 0), confirming a long range magnetic ordering in agreement with μ\muSR data. Our analysis of the magnetic structure reveals an ordered magnetic moment of 6.29(5)μB6.29(5)\,\mu_{\rm B} (at 1.8 K) on the Eu atoms and they form a ferromagnetic structure with moments aligned along the cc-axis. No change in the magnetic structure is observed in the reentrant or superconducting phases and the magnetic structure remains same for 1.8 K TTEu\leq T \leq T_{\rm Eu}. No clear evidence of structural transition or Fe moment ordering was found.Comment: 9 pages, 7 figures, to appear in Phys. Rev.

    New Scaling Variable at ISR Energies For P+P→ π ++ X Inclusive Reactions

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    Restricted Energy Loss Model in Ultraheavy Nuclei Charge Detection with SSNTD

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    Charged Multiplicity Distribution and its Bose Type Nature

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    Investigation of Superconducting Gap Structure in HfIrSi using muon spin relaxation/rotation

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    Appearance of strong spin-orbit coupling (SOC) is apparent in ternary equiatomic compounds with 5dd-electrons due to the large atomic radii of transition metals. SOC plays a significant role in the emergence of unconventional superconductivity. Here we examined the superconducting state of HfIrSi using magnetization, specific heat, zero and transverse-field (ZF/TF) muon spin relaxation/rotation (μ\muSR) measurements. Superconductivity is observed at TCT_\mathrm{C} = 3.6 K as revealed by specific heat and magnetization measurements. From the TFμ-\muSR analysis it is clear that superfluid density well described by an isotropic BCS type ss-wave gap structure. Furthermore, from TFμ-\muSR data we have also estimated the superconducting carrier density nsn_\mathrm{s} = 6.6 ×\times1026^{26}m3^{-3}, London penetration depth λL(0)\lambda_{L}(0) = 259.59 nm and effective mass mm^{*} = 1.57 mem_{e}. Our zero-field muon spin relaxation data indicate no clear sign of spontaneous internal field below TCT_\mathrm{C}, which implies that the time-reversal symmetry is preserved in HfIrSi. Theoretical investigation suggests Hf and Ir atoms hybridize strongly along the cc-axis of the lattice, which is responsible for the strong three-dimensionality of this system which screens the Coulomb interaction. As a result despite the presence of correlated dd-electrons in this system, the correlation effect is weakened, promoting electron-phonon coupling to gain importance.Comment: 8 pages, 4 figure
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