2,450 research outputs found

    Physical Mechanism of the d->d+is Transition

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    We discuss the basic physical mechanism of the d->d+is transition, which is the currently accepted explanation for the results of tunneling experiments into abab planes. Using the first-order perturbation theory, we show that the zero-bias states drive the transition. We present various order-of-magnitude estimates and consistency checks that support this picture.Comment: 7 pages, 2 figure

    Bootstrapping 3D Fermions with Global Symmetries

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    We study the conformal bootstrap for 4-point functions of fermions ψiψjψkψ\langle \psi_i \psi_j \psi_k \psi_{\ell} \rangle in parity-preserving 3d CFTs, where ψi\psi_i transforms as a vector under an O(N)O(N) global symmetry. We compute bounds on scaling dimensions and central charges, finding features in our bounds that appear to coincide with the O(N)O(N) symmetric Gross-Neveu-Yukawa fixed points. Our computations are in perfect agreement with the 1/N1/N expansion at large NN and allow us to make nontrivial predictions at small NN. For values of NN for which the Gross-Neveu-Yukawa universality classes are relevant to condensed-matter systems, we compare our results to previous analytic and numerical results.Comment: 29 pages, 7 figure

    Bootstrapping 3D Fermions

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    We study the conformal bootstrap for a 4-point function of fermions ψψψψ\langle\psi\psi\psi\psi\rangle in 3D. We first introduce an embedding formalism for 3D spinors and compute the conformal blocks appearing in fermion 4-point functions. Using these results, we find general bounds on the dimensions of operators appearing in the ψ×ψ\psi \times \psi OPE, and also on the central charge CTC_T. We observe features in our bounds that coincide with scaling dimensions in the Gross-Neveu models at large NN. We also speculate that other features could coincide with a fermionic CFT containing no relevant scalar operators.Comment: 45 pages, 8 figures; V2: added references and small clarifications to match JHEP versio

    Fermion-Scalar Conformal Blocks

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    We compute the conformal blocks associated with scalar-scalar-fermion-fermion 4-point functions in 3D CFTs. Together with the known scalar conformal blocks, our result completes the task of determining the so-called `seed blocks' in three dimensions. Conformal blocks associated with 4-point functions of operators with arbitrary spins can now be determined from these seed blocks by using known differential operators.Comment: 25 pages; V2: added small clarifications to match JHEP versio

    Construction and measurements of a vacuum-swing-adsorption radon-mitigation system

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    Long-lived alpha and beta emitters in the 222^{222}Rn decay chain on (and near) detector surfaces may be the limiting background in many experiments attempting to detect dark matter or neutrinoless double-beta decay, and in screening detectors. In order to reduce backgrounds from radon-daughter plate-out onto the wires of the BetaCage during its assembly, an ultra-low-radon cleanroom is being commissioned at Syracuse University using a vacuum-swing-adsorption radon-mitigation system. The radon filter shows ~20×\times reduction at its output, from 7.47±\pm0.56 to 0.37±\pm0.12 Bq/m3^3, and the cleanroom radon activity meets project requirements, with a lowest achieved value consistent with that of the filter, and levels consistently < 2 Bq/m3^3.Comment: 5 pages, 3 figures, Proceedings of Low Radioactivity Techniques (LRT) 2013, Gran Sasso, Italy, April 10-12, 201

    Morphological Characteristics of Meckel-Gruber Syndrome

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    Status of BetaCage: an Ultra-sensitive Screener for Surface Contamination

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    BetaCage, a gaseous neon time-projection chamber, has been proposed as a viable screener for emitters of low-energy alphas and electrons to which commercial radioactivity counting techniques are insensitive. Using radiopure materials for construction, active and passive shielding from extrinsic backgrounds, large counting area and minimal detector mass, BetaCage will be able to achieve sensitivities of 10^(−5) counts keV^(−1) kg^(−1) day^(−1) in a few days of running time. We report on progress in prototype development work since the last meeting of this workshop
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