401 research outputs found

    Anisotropic Compactification of Nonrelativistic M-Theory

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    We study a decoupling limit of M-theory where the three-form gauge potential becomes critical. This limit leads to nonrelativistic M-theory coupled to a non-Lorentzian spacetime geometry. Nonrelativistic M-theory is U-dual to M-theory in the discrete light cone quantization, a non-perturbative approach related to the Matrix theory description of M-theory. We focus on the compactification of nonrelativistic M-theory over a two-torus that exhibits anisotropic behaviors due to the foliation structure of the spacetime geometry. We develop a frame covariant formalism of the toroidal geometry, which provides a geometrical interpretation of the recently discovered polynomial realization of SL(2,Z) duality in nonrelativistic type IIB superstring theory. We will show that the nonrelativistic IIB string background fields transform as polynomials of an effective Galilean "boost velocity" on the two-torus. As an application, we construct an action principle describing a single M5-brane in nonrelativistic M-theory and study its compactification over the anisotropic two-torus. This procedure leads to a D3-brane action in nonrelativistic IIB string theory that makes the SL(2,Z) invariance manifest in the polynomial realization.Comment: 44 page

    Root-TTT \overline{T} Deformed Boundary Conditions in Holography

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    We develop the holographic dictionary for pure AdS3\mathrm{AdS}_3 gravity where the Lagrangian of the dual 2d2d conformal field theory has been deformed by an arbitrary function of the energy-momentum tensor. In addition to the TTT \overline{T} deformation, examples of such functions include a class of marginal stress tensor deformations which are special because they leave the generating functional of connected correlators unchanged up to a redefinition of the source and expectation value. Within this marginal class, we identify the unique deformation that commutes with the TTT \overline{T} flow, which is the root-TTT \overline{T} operator, and write down the modified boundary conditions corresponding to this root-TTT \overline{T} deformation. We also identify the unique marginal stress tensor flow for the cylinder spectrum of the dual CFT which commutes with the inviscid Burgers' flow driven by TTT \overline{T}, and we propose this unique flow as a candidate root-TTT \overline{T} deformation of the energy levels. We study BTZ black holes in AdS3\mathrm{AdS}_3 subject to root-TTT \overline{T} deformed boundary conditions, and find that their masses flow in a way which is identical to that of our candidate root-TTT \overline{T} energy flow equation, which offers evidence that this flow is the correct one. Finally, we also obtain the root-TTT \overline{T} deformed boundary conditions for the gauge field in the Chern-Simons formulation of AdS3\mathrm{AdS}_3 gravity.Comment: 65 pages; LaTe

    Response of Fish Communities to Habitat Alteration in a Small Ozark Stream

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    From 1984 to 1986, the Arkansas Highway and Transportation Department reconstructed and upgraded a portion of St. Hwy. 123 west of St. Hwy.7 at Pelsor, Arkansas. As a result of the construction, portions of Haw Creek, Johnson County, Arkansas, a third order stream in the Boston Mountains Ecoregion, were straightened and channelized. In reconstructing specific stream reaches, stream banks were riprapped and vegetated, gabions constructed and positioned, stream substrates and pool-riffle ratios altered. Instream and riparian habitat and fish biomass and diversity in altered reaches were radically altered. Channelized reaches became wide and shallow, lacking overstory cover and pools. Substrate particle size changed from boulder/rubble to rubble/gravel/sand and velocity increased. Fish communities in channeled reaches simple; Campostoma anomalum, Notropis boops, and Etheostoma spectabile accounted for more than 80 percent of all fish captured. This represented a shift from piscivore and insectivorepiscivore to herbivore and insectivore dominated feeding guilds. Natural channel reaches had more complex fish communities and greater abundance of centrarchids and ictalurids, primarily deeper water groups. Immediately after channelization, altered reaches had a larger biomass than natural reaches (0.43-0.26 g/m^2 ). The summer following alteration, channeled segments were basically dewatered, and biomass decreased dramatically (0.06-0.1 1 g/m^2). One year post channelization, altered reaches had eroded, scoured and deepened at their headwaters, and embedded. Fish community composition in altered reaches s stabilizing to a riffle-type assemblage dominated by the herbivore Campostoma anomalum

    TTT\overline{T} deformation in SCFTs and integrable supersymmetric theories

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    We calculate the S\mathcal{S}-multiplets for two-dimensional Euclidean N=(0,2)\mathcal{N}=(0,2) and N=(2,2)\mathcal{N} = (2,2) superconformal field theories under the TTT\overline{T} deformation at leading order of perturbation theory in the deformation coupling. Then, from these N=(0,2)\mathcal{N} = (0, 2) deformed multiplets, we calculate two- and three-point correlators. We show the N=(0,2)\mathcal{N} = (0,2) chiral ring's elements do not flow under the TTT\overline{T} deformation. For the case of N=(2,2)\mathcal{N} = (2,2), we show the twisted chiral ring and chiral ring cease to exist simultaneously. Specializing to integrable supersymmetric seed theories, such as N=(2,2)\mathcal{N} = (2,2) Landau-Ginzburg models, we use the thermodynamic Bethe ansatz to study the S-matrices and ground state energies. From both an S-matrix perspective and Melzer's folding prescription, we show that the deformed ground state energy obeys the inviscid Burgers' equation. Finally, we show that several indices independent of DD-term perturbations including the Witten index, Cecotti-Fendley-Intriligator-Vafa index and elliptic genus do not flow under the TTT\overline{T} deformation.Comment: 46 page

    Probing holography in pp-adic CFT

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    We holographically calculate the partition functions of CFTs dual to Bruhat-Tits trees and pp-adic BTZ black holes. Along the way, we propose new spectral decompositions of the Laplacian operator other than the plane-wave basis on these two types of backgrounds, with both analytical and numerical evidence. We extract the density of states and hence entropy from BTZ partition function via inverse Laplace transform. Then the one-loop Witten diagram is computed in the pp-adic BTZ black hole background, yielding constraints on the heavy-heavy-light averaged three-point coefficient of its boundary pp-adic CFT. Finally, for general pp-adic CFTs (not necessarily holographic), we analyze the representation theory of their global conformal group PGL(2,Qp)PGL\left(2,\mathbb{Q}_p\right), and discuss the suitability of different representations as Hilbert spaces of pp-adic CFT.Comment: 52 pages, 13 figure

    Spectroscopy of z ~ 7 candidate galaxies: using Lyman α to constrain the neutral fraction of hydrogen in the high-redshift universe

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    Following our previous spectroscopic observations of z > 7 galaxies with Gemini/Gemini Near Infra-Red Spectrograph (GNIRS) and Very Large Telescope (VLT)/XSHOOTER, which targeted a total of eight objects, we present here our results from a deeper and larger VLT/FOcal Reducer and Spectrograph (FORS2) spectroscopic sample of Wide Field Camera 3 selected z > 7 candidate galaxies. With our FORS2 setup we cover the 737–1070 nm wavelength range, enabling a search for Lyman α in the redshift range spanning 5.06–7.80. We target 22 z-band dropouts and find no evidence of Lyman α emission, with the exception of a tentative detection (<5σ, which is our adopted criterion for a secure detection) for one object. The upper limits on Lyman α flux and the broad-band magnitudes are used to constrain the rest-frame equivalent widths for this line emission. We analyse our FORS2 observations in combination with our previous GNIRS and XSHOOTER observations, and suggest that a simple model where the fraction of high rest-frame equivalent width emitters follows the trend seen at z = 3-6.5 is inconsistent with our non-detections at z ∼ 7.8 at the 96 per cent confidence level. This may indicate that a significant neutral H I fraction in the intergalactic medium suppresses Lyman α, with an estimated neutral fraction χHI∼0.5, in agreement with other estimates

    Etmopterus lailae Sp Nov., a New Lanternshark (Squaliformes: Etmopteridae) from the Northwestern Hawaiian Islands

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    A new species of lanternshark, Etmopterus lailae (Squaliformes: Etmopteridae), is described from the Northwestern Hawaiian Islands, in the central North Pacific Ocean. The new species resembles other members of the “Etmopterus lucifer” clade in having linear rows of dermal denticles, and most closely resembles E. lucifer from Japan. The new species occurs along insular slopes around seamounts at depths between 314–384 m. It can be distinguished from other members of the E. lucifer clade by a combination of characteristics, including a longer anterior flank marking branch, arrangement of dermal denticles on the ventral snout surface and body, flank and caudal markings, and meristic counts including number of spiral valve turns, and precaudal vertebrate. A key to species of the Etmopterus lucifer-clade is included

    Testing the Nature of the D_{sJ}^*(2317)^+ and D_{sJ}(2463)^+ States Using Radiative Transitions

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    The Babar and CLEO collaborations have recently observed states decaying to D_s^+\pi^0 and D_s^{*+}\pi^0 respectively and suggest the possible explanation that they are the missing P-wave c\bar{s} states with J^P=0^+ and 1^+. In this note we compare the properties of the D_{sJ}^*(2317)^+ and D_{sJ}(2463)^+ states to those expected of the c\bar{s} D_{s0}^* and D_{s1} states. We expect the D_{s0}^* and D_{s1} with the reported masses to be extremely narrow, \Gamma \sim {\cal O}(10\hbox{keV}), with large branching ratios to D^*_s\gamma for the D_{s0}^* and to D^*_s\gamma and D_s\gamma for the D_{s1}. Crucial to this interpretation of the Babar and CLEO observations is the measurement of the radiative transitions. We note that it may be possible to observe the Ds1(2536)D_{s1}(2536) in radiative transitions to the DsD_s^*.Comment: Major revisions to include recent observation by CLEO of D_{sJ}(2463)^+ including change of title and additional radiative transitions included in results. Conclusions are not change
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