arXiv subjects

T. Wiklind

Publications and source records attributed to T. Wiklind.

45 records · Page 3Linked to original sources

arXiv2000

IRAM observations of JVAS/CLASS gravitational lenses

We have searched for molecular absorption lines at millimeter wavelengths in eleven gravitational lens systems discovered in the JVAS/CLASS surveys of flat spectrum radio sources. Spectra of only one source 1030+074 were obtained in the 3-, 2- and 1.3-millimeter band at the frequencies corresponding to common molecular transitions of CO and HCO+ as continuum emission was not found in any of the other sources. We calculated upper limits to the column density in molecular absorption for 1030+074, using an excitation temperature of 15 K, to be N_{CO} < 6.3 x 10^{13} cm^{-2} and N_{HCO+} < 1.3 x 10^{11} cm^{-2}, equivalent to hydrogen column density of the order N_H < 10^{18} cm^{-2}, assuming standard molecular abundances. We also present the best upper limits of the continuum at the lower frequency for the other 10 gravitational lenses.

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arXiv1999

Distortion of the SED of High-z Luminous Infrared Galaxies by Strong Lensing

We present a model to estimate the effect of differential magnification on the SED of high-z ULIRGs. It is found that the ratio of the high temperature component to the low temperature component can vary with up to a factor of ten with source position on very small angular scales ~0.01". This means that a correction for differential magnification is needed when deriving dust properties from strongly lensed sources.

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arXiv1999

Time Delay of PKS1830-211 Using Molecular Absorption Lines

The use of molecular absorption lines in deriving the timde delay in PKS1830-211 is described, as well as results from a three year monitoring campaign. The time delay and the implied value for the Hubble constant are presented.

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arXiv1999

Detection of CO(4-3), CO(9-8), and dust emission in the BAL quasar APM 08279+5255 at a redshift of 3.9

We detected with the IRAM interferometer the lines of CO(4-3) and CO(9-8) from the recently-discovered broad absorption line quasar APM 08279+5255. The molecular lines are at a redshift of 3.911, which we take to be the true cosmological redshift of the quasar's host galaxy. This means the quasar emission lines at z=3.87 are blueshifted by a kinematic component of -2500 km/s, and, along with the broad absorption lines, are probably emitted in the quasar's wind or jet, moving toward us. The CO line ratios suggest the molecular gas is at a temperature of about 200 K, at a density of about 4000 cm^-3. We also detected the dust emission at 94 and 214 GHz (emitted wavelengths 650 and 290 microns). The spectral index of the mm/submm continuum is +3.2, indicating the dust emission is optically thin in this part of the spectrum. The extremely high CO and dust luminosities suggest magnification by gravitational lensing. Using the optical extent and our limit on the size of the CO region, we estimate a magnification of 7 to 30 for the CO lines and the far-IR continuum, and 14 to 60 for the optical/UV. In this interpretation, the molecular gas and dust is in a nuclear disk of radius 90 to 270 pc around the quasar. The quasar is 25 to 100 times stronger than, but otherwise resembles, the nucleus of Mrk 231.

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arXiv1998

Search for LiH in the ISM towards B0218+357

We report a tentative detection with the IRAM 30m telescope of the LiH molecule in absorption in front of the lensed quasar B0218+357. We have searched for the J = 0 -- 1 rotational line of lithium hydride at 444 GHz (redshifted to 263 GHz). The line, if detected, is optically thin, very narrow, and corresponds to a column density of N(LiH) = 1.6 10$^{12}$ cm$^{-2}$ for an assumed excitation temperature of 15 K, or a relative abundance LiH/H$_2 \sim$ 3 10$^{-12}$. We discuss the implications of this result.

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arXiv1997

Molecular lines in absorption: recent results

Some recent results are presented about high redshift molecular absorption lines, namely about chemical abundances of elements, and in particular of water and molecular oxygen. Excitation temperatures of several molecules are found lower than the cosmic background temperature at the corresponding redshift z=0.88582 in PKS1830-211, and interpretations are proposed. The radio flux monitoring of the two gravitational images of PKS1830-211 is presented over almost two years, but precise calibration is still preventing the determination of the time-delay without ambiguity. The high spectral resolution of radio observations allows to put constraints on the variation of the fine-structure constant over a large fraction of the Hubble time.

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arXiv1997

New upper limits on the interstellar O2 abundance

We report new observations of molecular oxygen in absorption at z=0.685 in front of the radio source B0218+357. The lines at 56.3 and 118.7 GHz have been observed, redshifted to 33.4 and 70.5 GHz respectively, with the 12m at Kitt Peak, 43m at Green Bank telescopes, and the 45m Nobeyama radio telescope. Deriving the surface filling factor of the absorbing dark cloud with other lines detected at nearby frequencies, we deduce from the upper limits on the O2 lines a relative abundance of molecular oxygen with respect to carbon monoxyde of O2/CO $\la$ 2 10$^{-3}$ at 1$σ$, seven times lower than the previous limit. The consequences of this result are discussed.

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arXiv1997

Detection of water at z = 0.685 towards B0218+357

We report the detection of the H_2O molecule in absorption at a redshift z = 0.68466 in front of the gravitationally lensed quasar B0218+357. We detect the fundamental transition of ortho-water at 556.93 GHz (redshifted to 330.59 GHz). The line is highly optically thick and relatively wide (15 km/s FWHM), with a profile that is similar to that of the previously detected CO(2--1) and HCO^+(2--1) optically thick absorption lines toward this quasar. From the measured level of the continuum at 330.59 GHz, which corresponds to the level expected from the power-law spectrum $S(ν) \propto ν^{-0.25}$ already observed at lower frequencies, we deduce that the filling factor of the H_2O absorption is large. It was already known from the high optical thickness of the CO, ^{13}CO and C^{18}O lines that the molecular clouds entirely cover one of the two lensed images of the quasar (all its continuum is absorbed); our present results indicate that the H_2O clouds are covering a comparable surface. The H_2O molecules are therefore not confined to small cores with a tiny filling factor, but are extended over parsec scales. The H_2O line has a very large optical depth, and only isotopic lines could give us the water abundance. We have also searched for the 183 GHz line in absorption, obtaining only an upper limit; this yields constraints on the excitation temperature.

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arXiv1996

Search for molecular absorption in the tori of active galactic nuclei

We describe a search for molecular absorption at millimetre wavelengths associated with dusty molecular tori in active galactic nuclei (AGN). The sample observed consists of 11 flat-spectrum radio sources known to have red optical to infra-red colours plus two steep-spectrum narrow-line radio galaxies. Spectra of the sources were obtained in the 3-, 2- and 1.3-millimetre bands at frequencies corresponding to common molecular transitions of CO, HCO+, HCN and CS at the AGN redshift. No absorptions were detected in any of the sources. We calculated upper limits to the column density in molecular absorption, using an excitation temperature of 10 K, to be N(CO) < 10^{15} - 10^{16} cm^-2, equivalent to hydrogen columns of order N(H) < 10^{19} - 10^{20} cm^-2. These limits are significantly lower than the values N(H) \approx (2 - 6) 10^{21} cm^-2 that might be expected if the red colours of these sources were due to dust absorption at the quasar redshift as suggested by Webster et al. (1995). Should the excitation temperature of the molecular transitions be higher than 100K, the upper limits to the H2 column densities would be greater than those derived from the red colours. To explain the lack of molecular absorption we conclude that either the optical extinction takes place outside the host galaxy (along the line of sight), or the excitation temperature of the molecular transitions is very high, or the obscuration is not associated with significant amounts of cold molecular gas. It is quite possible that the hard X-ray flux from the central source of these AGN is strong enough to photo-dissociate the molecules.

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