65 research outputs found

    Noise reduction through joint processing of gravity and gravity gradient data

    Get PDF
    International audienceIn mineral and oil exploration, gravity gradient data can help to delineate small-scale features that cannot be retrieved from gravity measurements. Removing high-frequency noise while preserving the high-frequency real signal is one of the most challenging tasks associated with gravity gradi-ometry data processing. We present a method to reduce gravity and gravity gradient data noise when both are measured in the same area, based on a least-squares simultaneous inversion of observations and physical constraints, inferred from the gravity gradient tensor definition and its mathematical properties. Instead of handling profiles individually, our noise-reduction method uses simultaneously measured values of the tensor components and of gravity in the whole survey area, benefiting from all available information. Synthetic examples show that more than half of the random noise can be removed from all tensor components and nearly all the noise from the gravity anomaly without altering the high-frequency information. We apply our method to a set of marine gravity gradiometry data acquired by Bell Geospace in the Faroe-Shetland Basin to demonstrate its power to resolve small-scale features

    Decays of the ρ^(1−+)\hat\rho(1^{-+}) Exotic Hybrid and η\eta-ηâ€Č\eta' Mixing

    Full text link
    QCD sum-rules are used to calculate the ρ^(1−+)→πη,πηâ€Č\hat\rho(1^{-+})\to\pi\eta, \pi\eta' decay widths of the exotic hybrid in two different η−ηâ€Č\eta-\eta' mixing schemes. In the conventional flavour octet-singlet mixing scheme, the decay widths are both found to be small, while in the recently-proposed quark mixing scheme, the decay width Γρ^→ηπ≈250MeV\Gamma_{\hat\rho\to\eta\pi}\approx 250 MeV is large compared with the decay width Γρ^→ηâ€Čπ≈20MeV\Gamma_{\hat\rho\to\eta^\prime\pi}\approx 20 MeV. These results provide some insight into η\eta-ηâ€Č\eta' mixing and hybrid decay features.Comment: latex2e, 11 pages with 4 embedded eps figures. v 2 corrects reference [5] and minor error in equation (11

    Decay of heavy-light hybrids in HQET sum rules

    Full text link
    The decay widths of the 0^{++} and 1^{-+} heavy-light hybrids to B(D) and pion are calculated by using the QCD sum rules. The interpolated current of the hybrid is chosen as gqˉγαGαΌaTahv(x)g\bar q\gamma_{\alpha}G_{\alpha\mu}^aT^ah_{\it v}(x). In order to simplify the calculation and avoid the ambiguity of three-point correlation function, a two-point correlation function between the pion and vacuum is used instead. The decay width of the 0++→B(D)0^{++}\to B(D) is about 12(16) MeV while the 1−+→B(D)1^{-+}\to B(D) is around 0.4(1.8) MeV. We keep the leading order of 1/M_Q expansion in our calculation for convenience.Comment: 14 pages, latex file, 4 ps figs, Published version, some numerical results change

    Hybrid configuration content of heavy S-wave mesons

    Full text link
    We use the non-relativistic expansion of QCD (NRQCD) on the lattice to study the lowest hybrid configuration contribution to the ground state of heavy S-wave mesons. Using lowest-order lattice NRQCD to create the heavy-quark propagators, we form a basis of ``unperturbed'' S-wave and hybrid states. We then apply the lowest-order coupling of the quark spin and chromomagnetic field at an intermediate time slice to create ``mixed'' correlators between the S-wave and hybrid states. From the resulting amplitudes, we extract the off-diagonal element of our two-state Hamiltonian. Diagonalizing this Hamiltonian gives us the admixture of hybrid configuration within the meson ground state. The present effort represents a continuation of previous work: the analysis has been extended to include lattices of varying spacings, source operators having better overlap with the ground states, and the pseudoscalar (along with the vector) channel. Results are presented for bottomonium (΄\Upsilon, ηb\eta_b^{}) using three different sets of quenched lattices. We also show results for charmonium (J/ψJ/\psi, ηc\eta_c^{}) from one lattice set, although we note that the non-relativistic approximation is not expected to be very good in this case.Comment: 9 pages, 7 figures, version to appear in Phys Rev

    Can the Mechanism for π1→ηπ,ηâ€Čπ\pi_1\to \eta\pi,\eta'\pi Hybrid Decays be Detected?

    Full text link
    Two mechanisms for the π1\pi_1 (JPC=1−+J^{PC}=1^{-+}) hybrid meson decay processes π1→ηπ,ηâ€Čπ\pi_1\to\eta\pi,\eta'\pi are investigated. These mechanisms are applied to Ï•â†’Î·Îł,ηâ€ČÎł\phi\to\eta\gamma,\eta'\gamma and J/Ïˆâ†’Î·Îł,ηâ€ČÎłJ/\psi\to\eta\gamma,\eta'\gamma decays to illustrate the validity of the decay mechanisms and to obtain independent information on the coupling of η,ηâ€Č\eta,\eta' to quark and gluonic operators. From this information, we find that Γ(π1→ηπ)/Γ(π1→ηâ€Čπ)\Gamma(\pi_1\to\eta\pi)/\Gamma(\pi_1\to\eta'\pi) is substantially different in the two decay mechanisms, and hence future experimental measurements of this ratio will provide valuable information for substantiating the hybrid nature of these states and for determining the mechanism for these hybrid decays.Comment: 5 pages, revtex, 1 eps figure embedded in manuscript. Analysis and references extended in v

    A Study of the \eta \pi^{0} Spectrum and Search for a J^{PC} = 1^{-+} Exotic Meson

    Full text link
    A partial wave analysis (PWA) of the of the ηπ0\eta \pi ^0 system (where η→γγ\eta \to \gamma \gamma) produced in the charge exchange reaction π−p→ηπ0n\pi ^-p\to \eta \pi ^0n at an incident momentum of 18 GeV/c/c is presented as a function of ηπ0{\eta \pi ^0} invariant mass, mηπ0m_{\eta\pi^0}, and momentum transfer squared, tπ−→ηπt_{\pi^{-}\to\eta\pi}, from the incident π−\pi^- to the outgoing ηπ0{\eta\pi ^0} system. SS, PP and DD waves were included in the PWA. The a0(980)a_0(980) and a2(1320)a_2(1320) states are clearly observed in the overall ηπ0{\eta\pi ^0} effective mass distribution as well as in the amplitudes associated with SS wave and DD waves respectively after partial wave decomposition. The observed distributions in moments (averages of spherical harmonics) were compared to the results from the PWA and the two are consistent. The distribution in tπ−→ηπt_{\pi^{-}\to\eta\pi} for individual DD waves associated with natural and unnatural parity exchange in the tt-channel are consistent with Regge phenomenology. Of particular interest in this study is the PP wave since this leads to an exotic JPC=1−+J^{PC}=1^{-+} for the ηπ\eta \pi system. A PP wave is present in the data, however attempts to describe the mass dependence of the amplitude and phase motion with respect to the DD wave as a Breit-Wigner resonance are problematic. This has implications regarding the existence of a reported exotic JPC=1−+J^{PC} = 1^{-+} meson decaying into ηπ0\eta \pi^0 with a mass near 1.4 GeV/c2/c^2.Comment: 19 pages, 29 figures, to appear in Phys. Rev.

    NS3 protease polymorphism and natural resistance to protease inhibitors in French patients infected with HCV genotypes 1–5

    Get PDF
    Background: Resistant HCV populations may pre-exist in patients before NS3 protease inhibitor therapy and would likely be selected under specific antiviral pressure. The higher prevalence and lower rate of response to treatment associated with HCV genotype 1 infections has led to drug discovery efforts being focused primarily on enzymes produced by this genotype. Protease inhibitors may also be useful for non-genotype-1-infected patients, notably for non-responders.Methods: We investigated the prevalence of dominant resistance mutations and polymorphism in 298 HCV protease-inhibitor-naive patients infected with HCV genotypes 1, 2, 3, 4 or 5. Genotype-specific NS3 primers were designed to amplify and sequence the NS3 protease gene. Results: None of the 233 analysed sequences contained major telaprevir (TVR) or boceprevir (BOC) resistance mutations (R155K/T/M, A156S/V/T and V170A). Some substitutions (V36L, T54S, Q80K/R, D168Q and V170T) linked to low or moderate decreases in HCV sensitivity to protease inhibitors were prevalent according to genotype (between 2% and 100%). Other than genotype signature mutations at positions 36, 80 and 168, the most frequent substitution was T54S (4 genotype 1 and 2 genotype 4 sequences). All genotype 2–5 sequences had the non-genotype-1 signature V36L mutation known to confer low-level resistance to both TVR and BOC. Conclusions: We have developed an HCV protease NS3 inhibitor resistance genotyping tool suitable for use with HCV genotypes 1–5. Polymorphism data is valuable for interpreting genotypic resistance profiles in cases of failure of anti-HCV NS3 protease treatment

    Evidence for Exotic J^{PC}=1^{-+} Meson Production in the Reaction pi- p --> eta pi- p at 18 GeV/c

    Full text link
    Details of the analysis of the eta pi- system studied in the reaction pi^{-} p --> eta pi^{-} p at 18 GeV/c are given. Separate analyses for the 2 gamma and pi+ pi- pi0 decay modes of the eta are presented. An amplitude analysis of the data indicates the presence of interference between the a(2)(1320)- and a J^{PC}=1^{-+} wave between 1.2 and 1.6 GeV/c^2. The phase difference between these waves shows phase motion not attributable solely to the a(2)(1320)-. The data can be fitted by interference between the a(2)(1320)- and an exotic 1^{-+} resonance with M = 1370 +-16 +50 -30} MeV/c^2 and Gamma = 385 +- 40 +65 -105 MeV/c^2. Our results are compared with those of other experiments.Comment: 50 pages of text and 34 figure

    Interpretation of Experimental J^PC Exotic Signals

    Get PDF
    We investigate theoretical interpretations of the 1.4 GeV J^PC exotic resonance reported by the E852 collaboration. It is argued that interpretation in terms of a hybrid meson is untenable. A K-matrix analysis shows that the 1.4 GeV enhancement in the E852 eta pi data can be understood as an interference of a non-resonant Deck-type background and a resonance at 1.6 GeV. A final state rescattering calculation shows that the 1.6 GeV hybrid has a eta pi width which is bounded above by 57 \pm 14 MeV.Comment: 23 pages, LaTeX, 4 encapsulated postscript figures. Accepted for publication by Physical Review
    • 

    corecore