27,817 research outputs found
Johnston Atoll: reef fish hybrid zone between Hawaii and the equatorial Pacific
Johnston Atoll is isolated in the Central Pacific Ocean (16°45′ N 169°31′ W) about 1287 km (800 miles) southwest of Honolulu, Hawaii and 1440 km (900 miles) north of the equatorial Line Islands, Kiribati. The labrid species, Thalassoma lutescens, has a wide range of distribution in the equatorial Pacific. The related species, Thalassoma duperrey, is endemic to the Hawaiian Islands. The pelagic larvae of both species dispersed to Johnston Atoll, where we found a mix of adult phenotypes representing a range of hybridization events over generations. A hybrid acanthurid was also documented. In addition, the arrival and colonization of two pomacentrid (damselfish) species to the atoll was observed in 1999. These pomacentrid sister-species, Abudefduf abdominalis and A. vaigiensis, have become established populations with subsequent hybridization. The biogeography of the Johnston Atoll coral reef fish population shows some degree of local population retention. It is also evident that this biogeographic isolation is periodically compromised by large ocean current oscillations in the equatorial and central Pacific Ocean that bring larval fishes from either Hawaii or the Line Islands, and may distribute Johnston Atoll originating larvae elsewhere as well. The reef fauna and oceanography of this atoll provides the circumstances for improving scientific insight into marine fish speciation and island biogeography.Published versio
U.S. Extended Continental Shelf Cruise to Map Gaps in Kela and Karin Ridges, Johnston Atoll, Equatorial Pacific Ocean
The objectives for cruise KM14-17 are to map the bathymetry of two gaps in two submarine ridges in the vicinity of Johnston Atoll. One ridge gap occurs along the informally named Keli Ridge (Hein et al., 2005) south of Johnston Atoll and the other ridge gap occurs north of Johnston Atoll that separates Sculpin Ridge (also informally called Karin Ridge) and Horizon Ridge, all in the central equatorial Pacific (Fig. 1). The cruise took advantage of a scheduled dead-head transit from Papeete, Tahiti to Honolulu, Hawai’i that could be extended for 5 days to include the planned mapping. The mapping is in support of the U.S. (Extended Continental Shelf (ECS) Task Force. These areas were identified by the ECS Central Pacific Integrated Regional Team as having the potential for an ECS
The kilohertz quasi-periodic oscillations during the Z and atoll phases of the unique transient XTE J1701--462
We analysed 866 observations of the neutron-star low-mass X-ray binary XTE
J1701-462 during its 2006-2007 outburst. XTE J1701-462 is the only example so
far of a source that during an outburst showed, beyond any doubt, spectral and
timing characteristics both of the Z and atoll type. We found that the lower
kHz QPO in the atoll phase has a significantly higher coherence and fractional
rms amplitude than any of the kHz QPOs seen during the Z phase, and that in the
same frequency range, atoll lower kHz QPOs show coherence and fractional rms
amplitude, respectively, 2 and 3 times larger than the Z kHz QPOs. Out of the
707 observations in the Z phase, there is no single observation in which the
kHz QPOs have a coherence or rms amplitude similar to those seen when XTE
J1701-462 was in the atoll phase, even though the total exposure time was about
5 times longer in the Z than in the atoll phase. Since it is observed in the
same source, the difference in QPO coherence and rms amplitude between the Z
and atoll phase cannot be due to neutron-star mass, magnetic field, spin,
inclination of the accretion disk, etc. If the QPO frequency is a function of
the radius in the accretion disk in which it is produced, our results suggest
that in XTE J1701-462 the coherence and rms amplitude are not uniquely related
to this radius. Here we argue that this difference is instead due to a change
in the properties of the accretion flow around the neutron star. Regardless of
the precise mechanism, our result shows that effects other than the geometry of
space time around the neutron star have a strong influence on the coherence and
rms amplitude of the kHz QPOs, and therefore the coherence and rms amplitude of
the kHz QPOs cannot be simply used to deduce the existence of the innermost
stable circular orbit around a neutron star.Comment: 11 pages, 5 figures, 2 tables, submitted to MNRA
Terzan 5 transient IGR J17480-2446: variation of burst and spectral properties with spectral states
We study the spectral state evolution of the Terzan 5 transient neutron star
low-mass X-ray binary IGR J17480-2446, and how the best-fit spectral parameters
and burst properties evolved with these states, using the Rossi X-ray Timing
Explorer data. As reported by other authors, this is the second source which
showed transitions between atoll state and `Z' state. We find large scale
hysteresis in the almost `C'-like hardness-intensity track of the source in the
atoll state. This discovery is likely to provide a missing piece of the jigsaw
puzzle involving various types of hardness-intensity tracks from `q'-shaped for
Aquila X-1, 4U 1608-52, and many black holes to `C'-shaped for many atoll
sources. Furthermore, the regular pulsations, a diagonal transition between
soft and hard states, and the large scale hysteresis observed from IGR
J17480-2446 argue against some of the previous suggestions involving magnetic
field about atolls and millisecond pulsars. Our results also suggest that the
nature of spectral evolution throughout an outburst does not, at least
entirely, depend on the peak luminosity of the outburst. Besides, the source
took at least a month to trace the softer banana state, as opposed to a few
hours to a day, which is typical for an atoll source. In addition, while the
soft colour usually increases with intensity in the softer portion of an atoll
source, IGR J17480-2446 showed an opposite behaviour. From the detailed
spectral fitting we conclude that a blackbody+powerlaw model is the simplest
one, which describes the source continuum spectra well throughout the outburst.
We find that these two spectral components were plausibly connected with each
other, and they worked together to cause the source state evolution.
(Truncated).Comment: 16 pages, 8 figures, 2 tables, accepted for publication in MNRA
The kHz QPOs as a probe of the X-ray color-color diagram and accretion-disk structure for the atoll source 4U 1728-34
We have taken the kHz QPOs as a tool to probe the correlation between the
tracks of X-ray color-color diagram (CCD) and magnetosphere-disk positions for
the atoll source 4U 1728-34, based on the assumptions that the upper kHz QPO is
ascribed to the Keplerian orbital motion and the neutron star (NS)
magnetosphere is defined by the dipole magnetic field. We find that from the
island to the banana state, the inner accretion disk gradually approaches the
NS surface with the radius decreasing from r ~33.0km to ~15.9 km, corresponding
to the magnetic field from B(r) ~4.8*10^6 G to ~4.3*10^7 G. In addition, we
note the characteristics of some particular radii of magnetosphere-disk -r are:
firstly, the whole atoll shape of the CCD links the disk radius range of ~15.9
- 33.0 km, which is just located inside the corotation radius of 4U 1728-34
-r_co ( ~34.4 km), implying that the CCD shape is involved in the NS spin-up
state. Secondly, the island and banana states of CCD correspond to the two
particular boundaries: (I)-near the corotation radius at r ~27.2 - 33.0 km,
where the source lies in the island state; (II)-near the NS surface at r ~15.9
- 22.3 km, where the source lies in both the island and banana states. Thirdly,
the vertex of the atoll shape in CCD, where the radiation transition from the
hard to soft photons occurs, is found to be near the NS surface at r ~16.4 km.
The above results suggest that both the magnetic field and accretion
environment are related to the CCD structure of atoll track, where the
corotation radius and NS hard surface play the significant roles in the
radiation distribution of atoll source.Comment: 6 pages, 3 figures, 1 table, accepted by Astronomy & Astrophysic
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