Publications by authors named "CL Carilli"

We demonstrate the shape-orientation-size conservation principle for a three-element interferometer using aperture plane masking at the ALBA visible synchrotron radiation light source. We then use these data to demonstrate image plane self-calibration.

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  • - Galaxy clusters are huge structures containing thousands of galaxies and a hot intracluster medium (ICM), which makes up much of their mass and changes over time due to matter accumulation and mergers with other clusters.
  • - Previous observations of the ICM have mostly focused on older clusters, leaving a gap in understanding the ICM during the formation of the first massive clusters.
  • - Recent detection of the thermal Sunyaev-Zeldovich effect in the Spiderweb protocluster shows the presence of a nascent ICM about 10 billion years ago, revealing a less intense signal than expected, indicating a younger, active cluster formation phase.
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We develop a process of image-plane self-calibration for interferometric imaging data. The process is based on shape-orientation-size (SOS) conservation for the principal triangle in an image generated from the three fringes made from a triad of receiving elements, in situations where interferometric phase errors can be factorized into element-based terms. The basis of the SOS conservation principle is that, for a three-element array, the only possible image corruption due to an element-based phase screen is a tilt of the aperture plane, leading to a shift in the image plane.

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Distortions of the observed cosmic microwave background provide a direct measurement of the microwave background temperature at redshifts from 0 to 1 (refs. ). Some additional background temperature estimates exist at redshifts from 1.

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  • Detecting neutral hydrogen (H i) through 21 cm line emission is crucial for studying the universe's reionization phase, especially at redshifts greater than 6, but is complicated by strong foreground signals from other cosmic sources.
  • The proposed method utilizes interferometric bispectrum phase measurements, which are less affected by calibration errors, allowing researchers to differentiate between the H i signal and the brighter foreground emissions effectively.
  • This approach not only enhances the detection of the H i signal from the intergalactic medium but will also be beneficial for similar studies in other cosmic research areas, such as baryon acoustic oscillations.
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  • Researchers have been studying gas around high-redshift galaxies by looking at absorption line systems related to background quasars, but identifying the faint galaxies linked to them has been challenging.
  • Using the Atacama Large Millimeter/Submillimeter Array, the team successfully detected specific emissions from two galaxies connected to absorbers at a redshift of approximately 4.
  • Their findings suggest that these galaxies, which have high metallicity, share characteristics with massive star-forming galaxies and are surrounded by extended reservoirs of enriched neutral hydrogen gas.
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The largest galaxies in the universe reside in galaxy clusters. Using sensitive observations of carbon monoxide, we show that the Spiderweb galaxy-a massive galaxy in a distant protocluster-is forming from a large reservoir of molecular gas. Most of this molecular gas lies between the protocluster galaxies and has low velocity dispersion, indicating that it is part of an enriched intergalactic medium.

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  • - The most distant known quasars, found at redshift z approximately 6, appear to be evolved objects that are surprisingly similar to lower-redshift quasars, despite the Universe being only about 7% of its current age at that time.
  • - A recent study discovered a second quasar without emissions from hot dust, raising questions about whether this is a unique case or indicative of a broader trend at high redshift.
  • - Findings suggest that these high-redshift quasars, like the two without hot-dust emission, are in an early stage of evolution, growing rapidly with their central black holes, and likely formed in dust-free environments, indicating they haven't had time to accumulate hot dust.
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We have detected the four 18 cm OH lines from the z approximaetely 0.765 gravitational lens toward PMN J0134-0931. The 1612 and 1720 MHz lines are in conjugate absorption and emission, providing a laboratory to test the evolution of fundamental constants over a large lookback time.

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Images of the molecular CO 2-1 line emission and the radio continuum emission from the redshift 4.12 gravitationally lensed quasi-stellar object (QSO) PSS J2322+1944 reveal an Einstein ring with a diameter of 1.5".

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We present measurements of absorption by the 21 cm hyperfine transition of neutral hydrogen toward radio sources at substantial look-back times. These data are used in combination with observations of rotational transitions of common interstellar molecules to set limits on the evolution of the fine structure constant: alpha/ alpha<3.5x10(-15) yr(-1), to a look-back time of 4.

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We present detections of emission at 250 GHz (1.2 mm) from two high-redshift QSOs from the Sloan Digital Sky Survey sample using the bolometer array at the IRAM 30 m telescope. The sources are SDSSp 015048.

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Images of neutral hydrogen 21 cm absorption and radio continuum emission at 1.4 GHz from Mrk 273 were made using the Very Long Baseline Array and Very Large Array. These images reveal a gas disk associated with the northern nuclear region with a diameter 0&farcs;5 (370 pc) at an inclination angle of 53 degrees.

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We report observations of a luminous unresolved object at redshift z=4.62, with a featureless optical spectrum redward of the Lyalpha forest region, discovered from Sloan Digital Sky Survey commissioning data. The redshift is determined by the onset of the Lyalpha forest at lambda approximately 6800 Å and a Lyman limit system at lambda=5120 Å.

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Very-long-baseline interferometry images of the nuclear region of the radio galaxy Cygnus A reveal a pronounced "core" and a knotty jet and counterjet. The knots are moving away from the core at apparent speeds which are subluminal for h = 1 [h = H0/100 km.s-1.

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