9,239 research outputs found

    Induced antiferromagnetism and large magnetoresistances in RuSr2(Nd,Y,Ce)2Cu2O10-d ruthenocuprates

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    RuSr2(Nd,Y,Ce)2Cu2O10-d ruthenocuprates have been studied by neutron diffraction, magnetotransport and magnetisation measurements and the electronic phase diagram is reported. Separate Ru and Cu spin ordering transitions are observed, with spontaneous Cu antiferromagnetic order for low hole doping levels p, and a distinct, induced-antiferromagnetic Cu spin phase in the 0.02 < p < 0.06 pseudogap region. This ordering gives rise to large negative magnetoresistances which vary systematically with p in the RuSr2Nd1.8-xY0.2CexCu2O10-d series. A collapse of the magnetoresistance (MR) and magnetisation in the pre-superconducting region may signify the onset of superconducting fluctuations.Comment: 22 pages, 11 figure

    Examining c-di-GMP and possible quorum sensing regulation in Pseudomonas fluorescens SBW25:links between intra and inter-cellular regulation benefits community cooperative activities such as biofilm formation

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    Bacterial success in colonizing complex environments requires individual response to micro-scale conditions as well as community-level cooperation to produce large-scale structures such as biofilms. Connecting individual and community responses could be achieved by linking the intracellular sensory and regulatory systems mediated by bis-(3β€²-5β€²)-cyclic dimeric guanosine monophosphate (c-di-GMP) and other compounds of individuals with intercellular quorum sensing (QS) regulation controlling populations. There is growing evidence to suggest that biofilm formation by many pseudomonads is regulated by both intra and intercellular systems, though in the case of the model Pseudomonas fluorescens SBW25 Wrinkly Spreader in which mutations increasing c-di-GMP levels result in the production of a robust cellulose-based air-liquid interface biofilm, no evidence for the involvement of QS regulation has been reported. However, our recent review of the P. fluorescens SBW25 genome has identified a potential QS regulatory pathway and other QS–associated genes linked to c-di-GMP homeostasis, and QS signal molecules have also been identified in culture supernatants. These findings suggest a possible link between c-di-GMP and QS regulation in P. fluorescens SBW25 which might allow a more sophisticated and responsive control of cellulose production and biofilm formation when colonising the soil and plant-associated environments P. fluorescens SBW25 normally inhabits.Анализ Ρ†-Π΄ΠΈ-Π“ΠœΠ€ ΠΈ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΠ³ΠΎ чувства ΠΊΠ²ΠΎΡ€ΡƒΠΌΠ° Ρƒ Pseudomonas fluorescens SBW 25: связь ΠΌΠ΅ΠΆΠ΄Ρƒ Π²Π½ΡƒΡ‚Ρ€ΠΈ ΠΈ ΠΌΠ΅ΠΆΠΊΠ»Π΅Ρ‚ΠΎΡ‡Π½ΠΎΠΉ рСгуляциСй способствуСт ΠΊΠΎΠΎΠΏΠ΅Ρ€Π°Ρ‚ΠΈΠ²Π½ΠΎΠΌΡƒ повСдСнию Π² сообщСствС ΠΈ Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½ΠΈΡŽ Π±ΠΈΠΎΠΏΠ»Ρ‘Π½ΠΊΠΈΠ£ΡΠΏΠ΅ΡˆΠ½ΠΎΡΡ‚ΡŒ Π±Π°ΠΊΡ‚Π΅Ρ€ΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ ΠΊΠΎΠ»ΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ слоТных экониш Ρ‚Ρ€Π΅Π±ΡƒΠ΅Ρ‚ ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡƒΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ ΠΎΡ‚Π²Π΅Ρ‚Π° Π½Π° измСнСния условий Π½Π° ΠΌΠΈΠΊΡ€ΠΎΡƒΡ€ΠΎΠ²Π½Π΅ Ρ€Π°Π²Π½ΠΎ ΠΊΠ°ΠΊ ΠΈ ΠΊΠΎΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ Π½Π° ΡƒΡ€ΠΎΠ²Π½Π΅ сообщСства для ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ†ΠΈΠΈ Ρ‚Π°ΠΊΠΈΡ… ΠΊΡ€ΡƒΠΏΠ½ΠΎ ΠΌΠ°ΡΡˆΡ‚Π°Π±Π½Ρ‹Ρ… структур ΠΊΠ°ΠΊ Π±ΠΈΠΎΠΏΠ»Ρ‘Π½ΠΊΠΈ. ΠšΠΎΠΎΡ€Π΄ΠΈΠ½Π°Ρ†ΠΈΡ ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡƒΠ°Π»ΡŒΠ½Ρ‹Ρ… ΠΎΡ‚Π²Π΅Ρ‚ ΠΎΠ² ΠΈ ΠΎΡ‚Π²Π΅Ρ‚ΠΎΠ² сообщСства ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ достигнута ΠΏΡƒΡ‚Π΅ΠΌ связывания Π²Π½ΡƒΡ‚Ρ€ΠΈΠΊΠ»Π΅Ρ‚ΠΎΡ‡Π½Ρ‹Ρ… сСнсорных ΠΈ рСгуляторных систСм, опосрСдуСмых бис-(3',5')-цикличСским Π΄ΠΈΠΌΠ΅Ρ€Π½Ρ‹ΠΌ гуанозинмонофосфатом (Ρ†-Π΄ΠΈ-Π“ΠœΠ€) ΠΈ Π΄Ρ€ΡƒΠ³ΠΈΠΌΠΈ соСдинСниями ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡƒΡƒΠΌΠΎΠ² с ΠΌΠ΅ΠΆΠΊΠ»Π΅Ρ‚ΠΎΡ‡Π½ΠΎΠΉ рСгуляциСй - чувством ΠΊΠ²ΠΎΡ€ΡƒΠΌΠ° (ЧК), ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΠΈΡ€ΡƒΡŽΡ‰Π΅ΠΌ популяци ю. НакапливаСтся всё большС Π΄ΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»ΡŒΡΡ‚Π² Ρ‚ΠΎΠ³ΠΎ, Ρ‡Ρ‚ΠΎ Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ Π±ΠΈΠΎΠΏΠ»Π΅Π½ΠΊΠΈ ΠΌΠ½ΠΎΠ³ΠΈΠΌΠΈ псСвдомонадами рСгулируСтся ΠΊΠ°ΠΊ Π²Π½ΡƒΡ‚Ρ€ΠΈ ΠΊΠ»Π΅Ρ‚ΠΎΡ‡Π½Ρ‹ΠΌΠΈ, Ρ‚Π°ΠΊ ΠΈ ΠΌΠ΅ΠΆ ΠΊΠ»Π΅Ρ‚ΠΎΡ‡Π½Ρ‹ΠΌΠΈ рСгуляторными систСмами, хотя Π² случаС модСльной Pseudomonas fluorescens SBW25 Wrinkly Spreader, Ρƒ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΉ ΠΌΡƒΡ‚Π°Ρ†ΠΈΠΈ, ΠΏΠΎΠ²Ρ‹ΡˆΠ°ΡŽΡ‰ ΠΈΠ΅ ΡƒΡ€ΠΎΠ²Π½ΠΈ Ρ†-Π΄ΠΈ-Π“ΠœΠ€, приводят ΠΊ созданию ΠΏΡ€ΠΎΡ‡Π½ΠΎΠΉ Ρ†Π΅Π»Π»ΡŽΠ»ΠΎΠ·Π½ΠΎΠΉ Π±ΠΈΠΎΠΏΠ»Ρ‘Π½ΠΊΠΈ Π½Π° Π³Ρ€Π°Π½ΠΈΡ†Π΅ Ρ€Π°Π·Π΄Π΅Π»Π° Ρ„Π°Π· Π²ΠΎΠ·Π΄ΡƒΡ…-ΠΆΠΈΠ΄ΠΊΠΎΡΡ‚ΡŒ, Π½Π΅ Π±Ρ‹Π»ΠΎ ΠΎΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½ΠΎ Π½ΠΈ ΠΊΠ° ΠΊΠΎΠ³ΠΎ ΡΠ²ΠΈΠ΄Π΅Ρ‚Π΅Π»ΡŒΡΡ‚Π²Π° вовлСчСния ΠΊΠ²ΠΎΡ€ΡƒΠΌ-зависимой рСгуляции. Однако наш Π½Π΅Π΄Π°Π²Π½ΠΈΠΉ ΠΎΠ±Π·ΠΎΡ€ Π³Π΅Π½ΠΎΠΌΠ° P. fluorescens SBW25 выявил ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΉ ЧК-зависимый рСгуляторный ΠΏΡƒ Ρ‚ΡŒ ΠΈ Π΄Ρ€ΡƒΠ³ΠΈΠ΅ ЧК-зависимыС Π³Π΅Π½Ρ‹, связанныС с гомСостазом Ρ†-Π΄ΠΈ-Π“ΠœΠ€, Π° ΠΌΠΎΠ»Π΅ΠΊΡƒΠ»Ρ‹ ЧК-сигналинга Π±Ρ‹Π»ΠΈ ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Ρ‹ Π² ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€Π΅. Π­Ρ‚ΠΈ Π΄Π°Π½Π½Ρ‹Π΅ ΡΠ²ΠΈΠ΄Π΅Ρ‚Π΅Π»ΡŒΡΡ‚Π²ΡƒΡŽΡ‚ ΠΎ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΠΉ связи ΠΌΠ΅ΠΆΠ΄Ρƒ Ρ†-Π΄ΠΈ-Π“ΠœΠ€-рСгуляциСй ΠΈ ЧК Ρƒ P. fluorescens SBW25, Ρ‡Ρ‚ΠΎ позволяСт Π±ΠΎΠ»Π΅Π΅ слоТный ΠΈ Π³ΠΈΠ±ΠΊΠΈΠΉ ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŒ Π½Π°Π΄ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ†ΠΈΠ΅ΠΉ Ρ†Π΅Π»Π»ΡŽΠ»ΠΎΠ·Ρ‹ ΠΈ ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈ Π΅ΠΌ Π±ΠΈΠΎΠΏΠ»Π΅Π½ΠΊΠΈ ΠΏΡ€ΠΈ ΠΊΠΎΠ»ΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΏΠΎΡ‡Π² ΠΈ экониш, aссоциированных с растСниям ΠΈ, - СстСствСнными срСдами обитания P. fluorescens SBW25

    X-Ray Observations of Black Widow Pulsars

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    We describe the first X-ray observations of five short orbital period (PB<1P_B < 1 day), Ξ³\gamma-ray emitting, binary millisecond pulsars. Four of these, PSRs J0023+0923, J1124βˆ’-3653, J1810+1744, and J2256βˆ’-1024 are `black-widow' pulsars, with degenerate companions of mass β‰ͺ0.1MβŠ™\ll0.1 M_{\odot}, three of which exhibit radio eclipses. The fifth source, PSR J2215+5135, is an eclipsing `redback' with a near Roche-lobe filling ∼\sim0.2 solar mass non-degenerate companion. Data were taken using the \textit{Chandra X-Ray Observatory} and covered a full binary orbit for each pulsar. Two pulsars, PSRs J2215+5135 and J2256βˆ’-1024, show significant orbital variability while PSR J1124βˆ’-3653 shows marginal orbital variability. The lightcurves for these three pulsars have X-ray flux minima coinciding with the phases of the radio eclipses. This phenomenon is consistent with an intrabinary shock emission interpretation for the X-rays. The other two pulsars, PSRs J0023+0923 and J1810+1744, are fainter and do not demonstrate variability at a level we can detect in these data. All five spectra are fit with three separate models: a power-law model, a blackbody model, and a combined model with both power-law and blackbody components. The preferred spectral fits yield power-law indices that range from 1.3 to 3.2 and blackbody temperatures in the hundreds of eV. The spectrum for PSR J2215+5135 shows a significant hard X-ray component, with a large number of counts above 2 keV, which is additional evidence for the presence of intrabinary shock emission and is similar to what has been detected in the low-mass X-ray binary to millisecond pulsar transition object PSR J1023+0038.Comment: 8 pages, 6 figures, 2 tables, submitted to Ap

    Phase Mixing of AlfvΓ©n Waves Near a 2D Magnetic Null Point

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    The propagation of linear AlfvΓ©n wave pulses in an inhomogeneous plasma near a 2D coronal null point is investigated. When a uniform plasma density is considered, it is seen that an initially planar AlfvΓ©n wavefront remains planar, despite the varying equilibrium AlfvΓ©n speed, and that all the wave collects at the separatrices. Thus, in the non-ideal case, these AlfvΓ©nic disturbances preferentially dissipate their energy at these locations. For a non-uniform equilibrium density, it is found that the AlfvΓ©n wavefront is significantly distorted away from the initially planar geometry, inviting the possibility of dissipation due to phase mixing. Despite this however, we conclude that for the AlfvΓ©n wave, current density accumulation and preferential heating still primarily occur at the separatrices, even when an extremely non-uniform density profile is considered

    Goals, Strategies and First Discoveries of AO327, the Arecibo All-Sky 327 MHz Drift Pulsar Survey

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    We report initial results from AO327, a drift survey for pulsars with the Arecibo telescope at 327 MHz. The first phase of AO327 will cover the sky at declinations of -1 to 28 degrees, excluding the region within 5 degrees of the Galactic plane, where high scattering and dispersion make low-frequency surveys sub-optimal. We record data from a 57 MHz bandwidth with 1024 channels and 125 us sampling time. The 60 s transit time through the AO327 beam means that the survey is sensitive to very tight relativistic binaries even with no acceleration searches. To date we have detected 44 known pulsars with periods ranging from 3 ms to 2.21 s and discovered 24 new pulsars. The new discoveries include three millisecond pulsars, three objects with periods of a few tens of milliseconds typical of young as well as mildly recycled pulsars, a nuller, and a rotating radio transient. Five of the new discoveries are in binary systems. The second phase of AO327 will cover the sky at declinations of 28 to 38 degrees. We compare the sensitivity and search volume of AO327 to the Green Bank North Celestial Cap survey and the GBT350 drift survey, both of which operate at 350 MHz.Comment: Accepted for publication in Ap

    Fission Cycling in Supernova Nucleosynthesis: Active-Sterile Neutrino Oscillations

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    We investigate nucleosynthesis in the supernovae post-core bounce neutrino-driven wind environment in the presence of active-sterile neutrino transformation. We consider active-sterile neutrino oscillations for a range of mixing parameters: vacuum mass-squared differences of 0.1 eV^2 < dm^2 < 100 eV^2, and vacuum mixing angles of sin^2(2 theta_v) > 10^-4. We find a consistent r-process pattern for a large range of mixing parameters that is in rough agreement with the halo star CS 22892-052 abundances and the pattern shape is determined by fission cycling. We find that the allowed region for the formation of the r-process peaks overlaps the LSND and NSBL (3+1) allowed region.Comment: 11 pages, 7 figures, Corrected Typo

    Pulsar J0453+1559: A Double Neutron Star System with a Large Mass Asymmetry

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    To understand the nature of supernovae and neutron star (NS) formation, as well as binary stellar evolution and their interactions, it is important to probe the distribution of NS masses. Until now, all double NS (DNS) systems have been measured to have a mass ratio close to unity (q β‰₯\geq 0.91). Here we report the measurement of the individual masses of the 4.07-day binary pulsar J0453+1559 from measurements of the rate of advance of periastron and Shapiro delay: The mass of the pulsar is 1.559(5) MβŠ™M_{\odot} and that of its companion is 1.174(4) MβŠ™M_{\odot}; q = 0.75. If this companion is also a neutron star (NS), as indicated by the orbital eccentricity of the system (e=0.11), then its mass is the smallest precisely measured for any such object. The pulsar has a spin period of 45.7 ms and a spin derivative of 1.8616(7) x10βˆ’1910^-19; from these we derive a characteristic age of ~ 4.1 x 10910^9 years and a magnetic field of ~ 2.9 x 10910^9 G,i.e, this pulsar was mildly recycled by accretion of matter from the progenitor of the companion star. This suggests that it was formed with (very approximately) its current mass. Thus NSs form with a wide range of masses, which is important for understanding their formation in supernovae. It is also important for the search for gravitational waves released during a NS-NS merger: it is now evident that we should not assume all DNS systems are symmetric

    New Discoveries from the Arecibo 327 MHz Drift Pulsar Survey Radio Transient Search

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    We present Clusterrank, a new algorithm for identifying dispersed astrophysical pulses. Such pulses are commonly detected from Galactic pulsars and rotating radio transients (RRATs), which are neutron stars with sporadic radio emission. More recently, isolated, highly dispersed pulses dubbed fast radio bursts (FRBs) have been identified as the potential signature of an extragalactic cataclysmic radio source distinct from pulsars and RRATs. Clusterrank helped us discover 14 pulsars and 8 RRATs in data from the Arecibo 327 MHz Drift Pulsar Survey (AO327). The new RRATs have DMs in the range 23.5βˆ’86.623.5 - 86.6 pc cmβˆ’3^{-3} and periods in the range 0.172βˆ’3.9010.172 - 3.901 s. The new pulsars have DMs in the range 23.6βˆ’133.323.6 - 133.3 pc cmβˆ’3^{-3} and periods in the range 1.249βˆ’5.0121.249 - 5.012 s, and include two nullers and a mode-switching object. We estimate an upper limit on the all-sky FRB rate of 10510^5 dayβˆ’1^{-1} for bursts with a width of 10 ms and flux density ≳83\gtrsim 83 mJy. The DMs of all new discoveries are consistent with a Galactic origin. In comparing statistics of the new RRATs with sources from the RRATalog, we find that both sets are drawn from the same period distribution. In contrast, we find that the period distribution of the new pulsars is different from the period distributions of canonical pulsars in the ATNF catalog or pulsars found in AO327 data by a periodicity search. This indicates that Clusterrank is a powerful complement to periodicity searches and uncovers a subset of the pulsar population that has so far been underrepresented in survey results and therefore in Galactic pulsar population models.Comment: 41 pages, 16 figures, 4 tables, accepted by ApJ; added minor corrections to final ApJ proo

    Single-photon single ionization of W+^{+} ions: experiment and theory

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    Experimental and theoretical results are reported for photoionization of Ta-like (W+^{+}) tungsten ions. Absolute cross sections were measured in the energy range 16 to 245 eV employing the photon-ion merged-beam setup at the Advanced Light Source in Berkeley. Detailed photon-energy scans at 100 meV bandwidth were performed in the 16 to 108 eV range. In addition, the cross section was scanned at 50 meV resolution in regions where fine resonance structures could be observed. Theoretical results were obtained from a Dirac-Coulomb R-matrix approach. Photoionization cross section calculations were performed for singly ionized atomic tungsten ions in their 5s25p65d4(5D)6sβ€…β€Š6DJ5s^2 5p^6 5d^4({^5}D)6s \; {^6}{\rm D}_{J}, JJ=1/2, ground level and the associated excited metastable levels with JJ=3/2, 5/2, 7/2 and 9/2. Since the ion beams used in the experiments must be expected to contain long-lived excited states also from excited configurations, additional cross-section calculations were performed for the second-lowest term, 5d^5 \; ^6{\rm S}_{J}, JJ=5/2, and for the 4^4F term, 5d^3 6s^2 \; ^4{\rm F}_{J}, with JJ = 3/2, 5/2, 7/2 and 9/2. Given the complexity of the electronic structure of W+^+ the calculations reproduce the main features of the experimental cross section quite well.Comment: 23 pages, 7 figures, 1 table: Accepted for publication in J. Phys. B: At. Mol. & Opt. Phy
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