Published April 20, 2012 | Version v1
Journal article

HIGH SPECTRAL RESOLUTION MEASUREMENT OF THE SUNYAEV–ZEL'DOVICH EFFECT NULL WITH Z-Spec

  • 1. Department of Physics, Mathematics and Astronomy, California Institute of Technology, Pasadena, CA 91125 (United States)
  • 2. Department of Physics and Astronomy, University of Pennsylvania, Philadelphia, PA 19104 (United States)
  • 3. Center for Astrophysics and Space Astronomy, University of Colorado, CASA 389-UCB, Boulder, CO 80303 (United States)
  • 4. School of Physics and Astronomy, Cardiff University, Cardiff CF24 3YB (United Kingdom)
  • 5. Department of Physics and Astronomy, University of Alabama, 206 Gallalee Hall Box 870324, Tuscaloosa, AL 35487 (United States)
  • 6. Observatories of the Carnegie Institution for Science, 813 Santa Barbara Street, Pasadena, CA 91101 (United States)
  • 7. North American ALMA Science Center, National Radio Astronomy Observatory, Charlottesville, VA 22901 (United States)

Description

The Sunyaev-Zel'dovich (SZ) effect spectrum crosses through a null where ΔTCMB = 0 near ν0 = 217 GHz. In a cluster of galaxies, ν0 can be shifted from the canonical thermal SZ effect value by corrections to the SZ effect scattering due to the properties of the inter-cluster medium. We have measured the SZ effect in the hot galaxy cluster RX J 1347.5 – 1145 with Z-Spec, an R ∼ 300 grating spectrometer sensitive between 185 and 305 GHz. These data comprise a high spectral resolution measurement around the null of the SZ effect and clearly exhibit the transition from negative to positive ΔTCMB over the Z-Spec band. The SZ null position is measured to be ν0 = 225.8 ± 2.5(stat.) ± 1.2(sys.) GHz, which differs from the canonical null frequency by 3.0σ and is evidence for modifications to the canonical thermal SZ effect shape. Assuming the measured shift in ν0 is due only to relativistic corrections to the SZ spectrum, we place the limit kTe = 17.1 ± 5.3 keV from the zero-point measurement alone. By simulating the response of the instrument to the sky, we are able to generate likelihood functions in {y0, Te, vpec} space. For vpec = 0 km s–1, we measure the best-fitting SZ model to be y0 = 4.6+0.6–0.9 × 10–4, Te,0 = 15.2+12–7.4 keV. When vpec is allowed to vary, a most probable value of vpec = + 450 ± 810 km s–1 is found.

Availability note (English)

Available from http://dx.doi.org/10.1088/0004-637X/749/2/114

Additional details

Identifiers

Publishing Information

Journal Title
Astrophysical Journal
Journal Volume
749
Journal Issue
2
Journal Page Range
[13 p.]
ISSN
0004-637X
CODEN
ASJOAB

INIS

Country of Publication
United States
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
43106444
Subject category
S79: ASTROPHYSICS, COSMOLOGY AND ASTRONOMY;
Descriptors DEI
BACKGROUND RADIATION; CORRECTIONS; GALAXIES; GALAXY CLUSTERS; RELATIVISTIC RANGE; RELICT RADIATION; RESOLUTION; SPECTRA; SPECTROMETERS
Descriptors DEC
ELECTROMAGNETIC RADIATION; ENERGY RANGE; MEASURING INSTRUMENTS; MICROWAVE RADIATION; RADIATIONS