921 research outputs found
Probing the Active Massive Black Hole Candidate in the Center of NGC 404 with VLBI
Recently Nyland et al. (2012) argued that the radio emission observed in the
center of the dwarf galaxy NGC 404 originates in a low-luminosity active
galactic nucleus (LLAGN) powered by a massive black hole (
M). High-resolution radio detections of MBHs are rare. Here we
present sensitive, contemporaneous Chandra X-ray, and very long baseline
interferometry (VLBI) radio observations with the European VLBI Network (EVN).
The source is detected in the X-rays, and shows no long-term variability. If
the hard X-ray source is powered by accretion, the apparent low accretion
efficiency would be consistent with a black hole in the hard state. Hard state
black holes are known to show radio emission compact on the milliarcsecond
scales. However, the central region of NGC 404 is resolved out on 10
milliarcsecond (0.15-1.5 pc) scales. Our VLBI non-detection of a compact,
partially self-absorbed radio core in NGC 404 implies that either the black
hole mass is smaller than M, or the source
does not follow the fundamental plane of black hole activity relation. An
alternative explanation is that the central black hole is not in the hard
state. The radio emission observed on arcsecond (tens of pc) scales may
originate in nuclear star formation or extended emission due to AGN activity,
although the latter would not be typical considering the structural properties
of low-ionization nuclear emission-line region galaxies (LINERs) with confirmed
nuclear activity.Comment: Accepted for publication in the Astrophysical Journal. 7 pages, 2
figures, 1 tabl
A schematic model for QCD I: Low energy meson states
A simple model for QCD is presented, which is able to reproduce the meson
spectrum at low energy. The model is a Lipkin type model for quarks coupled to
gluons. The basic building blocks are pairs of quark-antiquarks coupled to a
definite flavor and spin. These pairs are coupled to pairs of gluons with spin
zero. The multiplicity problem, which dictates that a given experimental state
can be described in various manners, is removed when a particle-mixing
interaction is turned on. In this first paper of a series we concentrates on
the discussion of meson states at low energy, the so-called zero temperature
limit of the theory. The treatment of baryonic states is indicated, also.Comment: 29 pages, 6 figures. submitted to Phys. Rev.
Clusterization in the shape isomers of the 56Ni nucleus
The interrelation of the quadrupole deformation and clusterization is investigated in the example of the 56Ni nucleus. The shape isomers, including superdeformed and hyperdeformed states, are obtained as stability regions of the quasidynamical U(3) symmetry based on a Nilsson calculation. Their possible binary clusterizations are investigated by considering both the consequences of the Pauli exclusion principle and the energetic preference
The XMM-Newton Slew view of IGRJ17361-4441: a transient in the globular cluster NGC 6388
IGRJ17361-4441 is a hard transient recently observed by the INTEGRAL
satellite. The source, close to the center of gravity of the globular cluster
NGC 6388, quickly became the target of follow-up observations conducted by the
Chandra, Swift/XRT and RXTE observatories. Here, we concentrate in particular
on a set of observations conducted by the XMM-Newton satellite during two
slews, in order to get the spectral information of the source and search for
spectral variations. The spectral parameters determined by the recent
XMM-Newton slew observations were compared to the previously known results. The
maximum unabsorbed -ray flux in the 0.5-10 keV band as detected by the
XMM-Newton slew observations is erg cm
s, i.e. consistent with that observed by the Swift/XRT satellite 15 days
earlier. The spectrum seems to be marginally consistent () with that derived from the previous high energy observation.Comment: Accepted for publication on New Astronomy, 2012. A sentence about the
globular cluster 47 Tuc was partially rewritten to avoid confusio
Estimation of Nuclear DNA Content in Some Aegilops Species: Best Analyzed Using Flow Cytometry
The genera Triticum and Aegilops have been considered as the main gene pool of wheat due to their features, such as tolerance of all types of abiotic and biotic stresses. This study was conducted to evaluate the cytogenetic analyses in 115 native and wild populations from eleven Aegilops species using their nuclear DNA quantification. Mean 2C nuclear DNA contents of different ploidy levels in the wild wheat of Turkey and Iran were measured using the flow cytometry technique. The obtained results showed that the mean nuclear DNA content in diploid species varied from 10.09 pg/2C (Ae. umbellulata) to 10.95 pg/2C (Ae. speltoides var. ligustica) in Turkey. In Iranian diploids, the mean nuclear DNA content varied from 10.20 pg/2C (Ae. taushii) to 11.56 pg/2C (Ae. speltoides var. ligustica). This index in the tetraploid species of Turkey varied from 18.09 pg/2C (Ae. cylindrica) to 21.65 pg/2C (Ae. triaristata), and in Iranian species, it was from 18.61 pg/2C (Ae. cylindrica) to 21.75 pg/2C (Ae. columnaris). On the other hand, in the hexaploid species of Turkey, this index varied from 31.59 pg/2C (Ae. crassa) to 31.81 pg/2C (Ae. cylindrica); in the Iranian species, it varied from 32.58 pg/2C (Ae. cylindrica) to 33.97 pg/2C (Ae. crassa). There was a significant difference in the DNA content of Turkey and Iran diploid as well as tetraploid species; however, in hexaploid species, the difference was not significant. It was concluded that the variation in intraspecific genome size was very low in diploid and tetraploid populations; this means that the low variation is not dependent on geographic and climatic parameters. On the other hand, the interspecific variation is significant at the diploid and tetraploid populations. It is generally very difficult to distinguish Aegilops species from each other in natural conditions; meanwhile, in this study, all species could be, easily, quickly and unambiguously, distinguished and separated using the FCM technique
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