68,238 research outputs found

    Gravitationally enhanced depolarization of ultracold neutrons in magnetic-field gradients

    Get PDF
    Trapped ultracold neutrons (UCN) have for many years been the mainstay of experiments to search for the electric dipole moment (EDM) of the neutron, a critical parameter in constraining scenarios of new physics beyond the Standard Model. Because their energies are so low, UCN preferentially populate the lower region of their physical enclosure, and do not sample uniformly the ambient magnetic field throughout the storage volume. This leads to a substantial increase in the rate of depolarization, as well as to shifts in the measured frequency of the stored neutrons. Consequences for EDM measurements are discussed

    Unveiling Palomar 2: The Most Obscure Globular Cluster in the Outer Halo

    Get PDF
    We present the first color-magnitude study for Palomar 2, a distant and heavily obscured globular cluster near the Galactic anticenter. Our (V,V-I) color-magnitude diagram (CMD), obtained with the UH8K camera at the CFHT, reaches V(lim) = 24 and clearly shows the principal sequences of the cluster, though with substantial overall foreground absorption and differential reddening. The CMD morphology shows a well populated red horizontal branch with a sparser extension to the blue, similar to clusters such as NGC 1261, 1851, or 6229 with metallicities near [Fe/H] = -1.3.Fromanaverageofseveralindicators,weestimatetheforegroundreddeningatE(B−V)=1.24+−0.07andobtainatruedistancemodulus(m−M)0=17.1+−0.3. From an average of several indicators, we estimate the foreground reddening at E(B-V) = 1.24 +- 0.07 and obtain a true distance modulus (m-M)_0 = 17.1 +- 0.3, placing it about 34 kpc from the Galactic center. We use starcounts of the bright stars to measure the core radius, half-mass radius, and central concentration of the cluster. Its integrated luminosity is M_V = -7.9, making it clearly brighter and more massive than most other clusters in the outer halo.Comment: 25 pages, aastex, with 8 postscript figures; accepted for publication in AJ, September 1997. Also available by e-mail from [email protected]. Please consult Harris directly for (big) postscript files of Figures 1a,b (the images of the cluster

    Magnetic susceptibility of diluted pyrochlore and SCGO antiferromagnets

    Full text link
    We investigate the magnetic susceptibility of the classical Heisenberg antiferromagnet with nearest-neighbour interactions on the geometrically frustrated pyrochlore lattice, for a pure system and in the presence of dilution with nonmagnetic ions. Using the fact that the correlation length in this system for small dilution is always short, we obtain an approximate but accurate expression for the magnetic susceptibility at all temperatures. We extend this theory to the compound SrCr_{9-9x}Ga_{3+9x}O_{19} (SCGO) and provide an explanation of the phenomenological model recently proposed by Schiffer and Daruka [Phys. Rev. B56, 13712 (1997)].Comment: 4 pages, Latex, 4 postscript figures automatically include

    The Anomalous Hall Effect in YBa2_2Cu3_3O7_7

    Full text link
    The temperature dependence of the normal state Hall effect and magnetoresistance in YBa2_2Cu3_3O7_7 is investigated using the Nearly Antiferromagnetic Fermi Liquid description of planar quasiparticles. We find that highly anisotropic scattering at different regions of the Fermi surface gives rise to the measured anomalous temperature dependence of the resistivity and Hall coefficient while yielding the universal temperature dependence of the Hall angle observed for both clean and dirty samples. This universality is shown to arise from the limited momentum transfers available for the anomalous, spin fluctuation scattering and is preserved for any system with strong antiferromagnetic correlations.Comment: REVTeX, 10 pages + 4 figures in a single (compressed/uuencoded) PostScript fil

    Proposal for a [111] Magnetization Plateau in the Spin Liquid State of Tb2Ti2O7

    Full text link
    Despite a Curie-Weiss temperature θCW∼−14\theta_{\rm CW} \sim -14 K, the Tb2Ti2O7 pyrochlore magnetic material lacks long range magnetic order down to at least T∗≈50T^*\approx 50 mK. It has recently been proposed that the low temperature collective paramagnetic or spin liquid regime of this material may be akin to a spin ice state subject to both thermal and quantum fluctuations −- a {\it quantum spin ice} (QSI) of sorts. Here we explore the effect of a magnetic field B{\bm B} along the [111][111] direction on the QSI state. To do so, we investigate the magnetic properties of a microscopic model of Tb2Ti2O7 in an independent tetrahedron approximation in a finite B{\bm B} along [111][111]. Such a model describes semi-quantitatively the collective paramagnetic regime where nontrivial spin correlations start to develop at the shortest lengthscale, that is over a single tetrahedron, but where no long range order is yet present. Our results show that a magnetization plateau develops at low temperatures as the system develops B=0{\bm B}=0 ferromagnetic spin-ice-like "two-in/two-out" correlations at the shortest lengthscale. From these results, we are led to propose that the observation of such a [111] magnetization plateau in Tb2Ti2O7 would provide compelling evidence for a QSI at B=0{\bm B}=0 in this material and help guide the development of a theory for the origin of its spin liquid state.Comment: 6 pages, 3 figure

    Loneliness Across the Life Span

    Get PDF
    Most people have experienced loneliness and have been able to overcome it to reconnect with other people. In the current review, we provide a life-span perspective on one component of the evolutionary theory of loneliness—a component we refer to as the reaffiliation motive (RAM). The RAM represents the motivation to reconnect with others that is triggered by perceived social isolation. Loneliness is often a transient experience because the RAM leads to reconnection, but sometimes this motivation can fail, leading to prolonged loneliness. We review evidence of how aspects of the RAM change across development and how these aspects can fail for different reasons across the life span. We conclude with a discussion of age-appropriate interventions that may help to alleviate prolonged lonelines

    Dipolar Interactions and Origin of Spin Ice in Ising Pyrochlore Magnets

    Full text link
    Recent experiments suggest that the Ising pyrochlore magnets Ho2Ti2O7{\rm Ho_{2}Ti_{2}O_{7}} and Dy2Ti2O7{\rm Dy_{2}Ti_{2}O_{7}} display qualitative properties of the spin ice model proposed by Harris {\it et al.} \prl {\bf 79}, 2554 (1997). We discuss the dipolar energy scale present in both these materials and consider how they can display spin ice behavior {\it despite} the presence of long range interactions. Specifically, we present numerical simulations and a mean field analysis of pyrochlore Ising systems in the presence of nearest neighbor exchange and long range dipolar interactions. We find that two possible phases can occur, a long range ordered antiferromagnetic one and the other dominated by spin ice features. Our quantitative theory is in very good agreement with experimental data on both Ho2Ti2O7{\rm Ho_{2}Ti_{2}O_{7}} and Dy2Ti2O7{\rm Dy_{2}Ti_{2}O_{7}}. We suggest that the nearest neighbor exchange in Dy2Ti2O7{\rm Dy_{2}Ti_{2}O_{7}} is {\it antiferromagnetic} and that spin ice behavior is induced by long range dipolar interactions.Comment: 4 postscript figures included. Submitted to Physical Review Letters Contact: [email protected]

    Critical Dynamics of the Contact Process with Quenched Disorder

    Full text link
    We study critical spreading dynamics in the two-dimensional contact process (CP) with quenched disorder in the form of random dilution. In the pure model, spreading from a single particle at the critical point λc\lambda_c is characterized by the critical exponents of directed percolation: in 2+12+1 dimensions, δ=0.46\delta = 0.46, η=0.214\eta = 0.214, and z=1.13z = 1.13. Disorder causes a dramatic change in the critical exponents, to δ≃0.60\delta \simeq 0.60, η≃−0.42\eta \simeq -0.42, and z≃0.24z \simeq 0.24. These exponents govern spreading following a long crossover period. The usual hyperscaling relation, 4δ+2η=dz4 \delta + 2 \eta = d z, is violated. Our results support the conjecture by Bramson, Durrett, and Schonmann [Ann. Prob. {\bf 19}, 960 (1991)], that in two or more dimensions the disordered CP has only a single phase transition.Comment: 11 pages, REVTeX, four figures available on reques
    • …
    corecore