26,012 research outputs found

    Soft-Collinear Messengers: A New Mode in Soft-Collinear Effective Theory

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    It is argued that soft-collinear effective theory for processes involving both soft and collinear partons, such as exclusive B-meson decays, should include a new mode in addition to soft and collinear fields. These "soft-collinear messengers" can interact with both soft and collinear particles without taking them far off-shell. They thus can communicate between the soft and collinear sectors of the theory. The relevance of the new mode is demonstrated with an explicit example, and the formalism incorporating the corresponding quark and gluon fields into the effective Lagrangian is developed.Comment: 22 pages, 5 figures. Extended Section 6, clarifying the relevance of different types of soft-collinear interaction

    Phase Transitions in a Two-Component Site-Bond Percolation Model

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    A method to treat a N-component percolation model as effective one component model is presented by introducing a scaled control variable p+p_{+}. In Monte Carlo simulations on 16316^{3}, 32332^{3}, 64364^{3} and 1283128^{3} simple cubic lattices the percolation threshold in terms of p+p_{+} is determined for N=2. Phase transitions are reported in two limits for the bond existence probabilities p=p_{=} and pp_{\neq}. In the same limits, empirical formulas for the percolation threshold p+cp_{+}^{c} as function of one component-concentration, fbf_{b}, are proposed. In the limit p==0p_{=} = 0 a new site percolation threshold, fbc0.145f_{b}^{c} \simeq 0.145, is reported.Comment: RevTeX, 5 pages, 5 eps-figure

    Abnormal Perceptual Sensitivity in Body-Focused Repetitive Behaviors

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    Objective Several compulsive grooming habits such as hair pulling, skin picking, and nail biting are collectively known as body-focused repetitive behaviors (BFRBs). Although subclinical BFRBs are common and benign, more severe and damaging manifestations exist that are difficult to manage. Researchers have suggested that BFRBs are maintained by various cognitive, affective, and sensory contingencies. Although the involvement of cognitive and affective processes in BFRBs has been studied, there is a paucity of research on sensory processes. Methods The current study tested whether adults with subclinical or clinical BFRBs would report abnormal patterns of sensory processing as compared to a healthy control sample. Results Adults with clinical BFRBs (n = 26) reported increased sensory sensitivity as compared to persons with subclinical BFRBs (n = 48) and healthy individuals (n = 33). Elevations in sensation avoidance differentiated persons with clinical versus subclinical BFRBs. Sensation seeking patterns were not different between groups. Unexpectedly, BFRB severity was associated with lower registration of sensory stimuli, but this finding may be due to high psychiatric comorbidity rates in the BFRB groups. Conclusions These findings suggest that several sensory abnormalities may underlie BFRBs. Implications for the etiology and treatment of BFRBs are discussed

    Crossover from Single-Ion to Coherent Non-Fermi Liquid Behavior in Ce1x_{1-x}Lax_xNi9_9Ge4_4

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    We report specific heat and magneto-resistance studies on the compound Ce1x{}_{1-x}Lax{}_xNi9{}_9Ge4{}_4 for various concentrations over the entire stoichiometric range. Our data reveal single-ion scaling with Ce-concentration between x=0.1x = 0.1 and 0.95. Furthermore, CeNi9{}_9Ge4{}_4 turns out to have the largest ever recorded value of the electronic specific heat Δc/T\Delta c/T \approx 5.5 J K2mol1\rm K^{-2}mol^{-1} at T=0.08T=0.08 K which was found in Cerium f-electron lattice systems. In the doped samples Δc/T\Delta c/T increases logarithmically in the temperature range between 3 K and 50 mK typical for non-Fermi liquid (nFl) behavior, while ρ\rho exhibits a Kondo-like minimum around 30 K, followed by a single-ion local nFl behavior. In contrast to this, CeNi9{}_9Ge4{}_4 flattens out in Δc/T\Delta c/T below 300 mK and displays a pronounced maximum in the resistivity curve at 1.5 K indicating a coherent heavy fermion groundstate. These properties render the compound Ce1x{}_{1-x}Lax{}_xNi9{}_9Ge4{}_4 a unique system on the borderline between Fermi liquid and nFl physics.Comment: 2 pages, 3 figures, SCES0

    Shape-Function Effects and Split Matching in B-> Xs l+ l-

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    We derive the triply differential spectrum for the inclusive rare decay B -> Xs l+ l- in the shape function region, in which Xs is jet-like with mX2mbΛQCDmX^2 \lesssim mb \Lambda_QCD. Experimental cuts make this a relevant region. The perturbative and non-perturbative parts of the matrix elements can be defined with the Soft-Collinear Effective Theory, which is used to incorporate alphas corrections consistently. We show that, with a suitable power counting for the dilepton invariant mass, the same universal jet and shape functions appear as in B-> Xs gamma and B-> Xu l nu decays. Parts of the usual alphas(m_b) corrections go into the jet function at a lower scale, and parts go into the non-perturbative shape function. For B -> Xs l+ l-, the perturbative series in alphas are of a different character above and below mu=mb. We introduce a ``split matching'' method that allows the series in these regions to be treated independently.Comment: 33 pages; journal versio

    Size Matters: Origin of Binomial Scaling in Nuclear Fragmentation Experiments

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    The relationship between measured transverse energy, total charge recovered in the detector, and size of the emitting system is investigated. Using only very simple assumptions, we are able to reproduce the observed binomial emission probabilities and their dependences on the transverse energy.Comment: 14 pages, including 4 figure

    Spatially resolved ultrafast precessional magnetization reversal

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    Spatially resolved measurements of quasi-ballistic precessional magnetic switching in a microstructure are presented. Crossing current wires allow detailed study of the precessional switching induced by coincident longitudinal and transverse magnetic field pulses. Though the response is initially spatially uniform, dephasing occurs leading to nonuniformity and transient demagnetization. This nonuniformity comes in spite of a novel method for suppression of end domains in remanence. The results have implications for the reliability of ballistic precessional switching in magnetic devices.Comment: 17 pages (including 4 figures), submitted to Phys. Rev. Let
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