1,752 research outputs found

    Notes on the D=11D=11 pure spinor superparticle

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    The D=11D=11 pure spinor superparticle has been shown to describe linearized D=11D=11 supergravity in a manifestly covariant way. A number of authors have proposed that its correlation functions be used to compute amplitudes. The use of the scalar structure of the eleven-dimensional pure spinor top cohomology introduces a natural measure for computing such correlation functions. This prescription requires the construction of ghost number one and zero vertex operators. In these notes, we construct explicitly a ghost number one vertex operator but show the incompatibiliy of a ghost number zero vertex operator satisfying a standard descent equation for D=11D=11 supergravity.Comment: 13 page

    The Effect of the Defense Program on Scientific Research

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    Extended Infusion of Dexmedetomidine to an Infant at Sixty Times the Intended Rate

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    Dexmedetomidine is an α2 adrenergic agonist which has recently been approved in the United States for procedural sedation in adults. This report describes an infant who inadvertently received an intravenous infusion of dexmedetomidine at a rate which was 60 times greater than intended. We describe the hemodynamic, respiratory, and sedative effects of this overdose

    Dedication of the Palomar Observatory and the Hale Telescope

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    The dedication of the Palomar Observatory, if it were being held in England, would be accompanied by brilliant pageantry both of the state, with its knights, heralds, pursuivants, kings at arms, admirals and captains, and of the church with its bishops, priests and deacons, crucifiers and choirs; and I am sure that we feel the quality of religion in this ceremony. We would hear the choirs chanting in antiphony that great canticle which so delights the choir boys: Benedicite, omnia opera Domini

    A generalized study of the breeding potential of large heavy water moderated power reactors fueled with thoria and urania

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    "January 1967.""MIT-2073-5."Also issued as a Ph. D. thesis by the first author and supervised by the second and third authors, Massachusetts Institute of Technology, Dept. of Nuclear Engineering, 1966Includes bibliographical references (pages 324-328)U.S. Atomic Energy Commission contract AT(30-1)-207

    The Evolution of the Lyman-Alpha Luminosity Function During Reionization

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    The time frame in which hydrogen reionization occurred is highly uncertain, but can be constrained by observations of Lyman-alpha (Lyα\alpha) emission from distant sources. Neutral hydrogen in the intergalactic medium (IGM) attenuates Lyα\alpha~photons emitted by galaxies. As reionization progressed the IGM opacity decreased, increasing Lyα\alpha~visibility. The galaxy Lyα\alpha~luminosity function (LF) is thus a useful tool to constrain the timeline of reionization. In this work, we model the Lyα\alpha~LF as a function of redshift, z=510z=5-10, and average IGM neutral hydrogen fraction, \overline{x}_\textsc{hi}. We combine the Lyα\alpha~luminosity probability distribution obtained from inhomogeneous reionization simulations with a model for the UV LF to model the Lyα\alpha~LF. As the neutral fraction increases, the average number density of Lyα\alpha~emitting galaxies decreases, and are less luminous, though for \overline{x}_\textsc{hi} \lesssim 0.4 there is only a small decrease of the Lyα\alpha~LF. We use our model to infer the IGM neutral fraction at z=6.6,7.0,7.3z=6.6, 7.0, 7.3 from observed Lyα\alpha~LFs. We conclude that there is a significant increase in the neutral fraction with increasing redshift: \overline{x}_\textsc{hi}(z=6.6)=0.08^{+ 0.08}_{- 0.05}, \, \overline{x}_\textsc{hi}(z=7.0)=0.28 \pm 0.05 and \overline{x}_\textsc{hi}(z=7.3)=0.83^{+ 0.06}_{- 0.07}. We predict trends in the Lyα\alpha~luminosity density and Schechter parameters as a function of redshift and the neutral fraction. We find that the Lyα\alpha~luminosity density decreases as the universe becomes more neutral. Furthermore, as the neutral fraction increases, the faint-end slope of the Lyα\alpha~LF steepens, and the characteristic Lyα\alpha~luminosity shifts to lower values, concluding that the evolving shape of the Lyα\alpha~LF -- not just its integral -- is an important tool to study reionization.Comment: 20 pages, 10 figures, submitted to Ap

    Extended Infusion of Dexmedetomidine to an Infant at Sixty Times the Intended Rate

    Get PDF
    Dexmedetomidine is an α2 adrenergic agonist which has recently been approved in the United States for procedural sedation in adults. This report describes an infant who inadvertently received an intravenous infusion of dexmedetomidine at a rate which was 60 times greater than intended. We describe the hemodynamic, respiratory, and sedative effects of this overdose

    The Evolution of the Lyman-alpha Luminosity Function during Reionization

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    The time frame in which hydrogen reionization occurred is highly uncertain, but can be constrained by observations of Lyman-alpha (Lya) emission from distant sources. Neutral hydrogen in the intergalactic medium (IGM) attenuates Lya photons emitted by galaxies. As reionization progressed the IGM opacity decreased, increasing Lya visibility. The galaxy Lya luminosity function (LF) is thus a useful tool to constrain the timeline of reionization. In this work, we model the Lya LF as a function of redshift, z = 5 10, and average IGM neutral hydrogen fraction, xH?. We combine the Lya luminosity probability distribution obtained from inhomogeneous reionization simulations with a model for the UV LF to model the Lya LF. As the neutral fraction increases, the average number density of Lya emitting galaxies decreases, and are less luminous, though for xH? ? 0.4 there is only a small decrease in the Lya LF. We use our model to infer the IGM neutral fraction at z = 6.6, 7.0, and 7.3 from observed Lya LFs. We conclude that there is a significant increase in the neutral fraction with increasing redshift: = = - = = ? x z 6.6 0.08+ , x z 7.0 0.28 0.05 H 0.05 0.08 ? ( ) H? ( ) and = = - x z 7.3 0.83+ H 0.07 0.06 ? ( ) . We predict trends in the Lya luminosity density and Schechter parameters as a function of redshift and the neutral fraction. We find that the Lya luminosity density decreases as the universe becomes more neutral. Furthermore, as the neutral fraction increases, the faint-end slope of the Lya LF steepens, and the characteristic Lya luminosity shifts to lower values; hence, we conclude that the evolving shape of the Lya LF not just its integral is an important tool to study reionization
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