scholarly journals QUIJOTE scientific results – III. Microwave spectrum of intensity and polarization in the Taurus Molecular Cloud complex and L1527

2018 ◽  
Vol 486 (1) ◽  
pp. 462-485
Author(s):  
F Poidevin ◽  
J A Rubiño-Martín ◽  
C Dickinson ◽  
R Génova-Santos ◽  
S Harper ◽  
...  

Abstract We present new intensity and polarization observations of the Taurus Molecular Cloud (TMC) region in the frequency range 10–20 GHz with the multifrequency instrument (MFI) mounted on the first telescope of the Q-U-I-JOint TEnerife (QUIJOTE) experiment. From the combination of the QUIJOTE data with the WMAP 9-yr data release, the Planck second data release, the DIRBE maps, and ancillary data, we detect an anomalous microwave emission (AME) component with flux density $S_{\rm AME, peak} = 43.0 \pm 7.9\,$ Jy in the TMC and $S_{\rm AME, peak} = 10.7 \pm 2.7\,$ Jy in the dark cloud nebula L1527, which is part of the TMC. In the TMC the diffuse AME emission peaks around a frequency of 19 GHz, compared with an emission peak about a frequency of 25 GHz in L1527. In the TMC, the best constraint on the level of AME polarization is obtained at the Planck channel of 28.4 GHz, with an upper limit $\pi _{\rm AME}\lt 4.2\, {{\ \rm per\ cent}}$ (95 $\, {{\ \rm per\ cent}}$ C.L.), which reduces to $\pi _{\rm AME}\lt 3.8\, {{\ \rm per\ cent}}$ (95 $\, {{\ \rm per\ cent}}$ C.L.) if the intensity of all the free–free, synchrotron and thermal dust components are negligible at this frequency. The same analysis in L1527 leads to $\pi _{\rm AME}\lt 5.3{{\ \rm per\ cent}}$ (95 $\, {{\ \rm per\ cent}}$ C.L.) or $\pi _{\rm AME}\lt 4.5\, {{\ \rm per\ cent}}$ (95 ${{\ \rm per\ cent}}$ C.L.) under the same assumption. We find that in the TMC and L1527 on average about $80{{\ \rm per\ cent}}$ of the H ii gas should be mixed with thermal dust. Our analysis shows how the QUIJOTE-MFI 10–20 GHz data provide key information to properly separate the synchrotron, free–free, and AME components.

1991 ◽  
Vol 147 ◽  
pp. 505-507
Author(s):  
Shoba Veeraraghavan ◽  
Gary A. Fuller

Two topological tools for studying the global structure of molecular clouds, the genus and the contour-crossing statistic, are discussed. Preliminary results for the Taurus molecular cloud complex are presented.


2011 ◽  
Vol 739 (1) ◽  
pp. L4 ◽  
Author(s):  
Nirupam Roy ◽  
Abhirup Datta ◽  
Emmanuel Momjian ◽  
Anuj P. Sarma

1991 ◽  
Vol 147 ◽  
pp. 505-507
Author(s):  
Shoba Veeraraghavan ◽  
Gary A. Fuller

Two topological tools for studying the global structure of molecular clouds, the genus and the contour-crossing statistic, are discussed. Preliminary results for the Taurus molecular cloud complex are presented.


Author(s):  
Simon Casassus ◽  
Matías Vidal ◽  
Carla Arce-Tord ◽  
Clive Dickinson ◽  
Glenn J White ◽  
...  

Abstract Cm-wavelength radio continuum emission in excess of free-free, synchrotron and Rayleigh-Jeans dust emission (excess microwave emission, EME), and often called ‘anomalous microwave emission’, is bright in molecular cloud regions exposed to UV radiation, i.e. in photo-dissociation regions (PDRs). The EME correlates with IR dust emission on degree angular scales. Resolved observations of well-studied PDRs are needed to compare the spectral variations of the cm-continuum with tracers of physical conditions and of the dust grain population. The EME is particularly bright in the regions of the ρ Ophiuchi molecular cloud (ρ Oph) that surround the earliest type star in the complex, HD 147889, where the peak signal stems from the filament known as the ρ Oph-W PDR. Here we report on ATCA observations of ρ Oph-W that resolve the width of the filament. We recover extended emission using a variant of non-parametric image synthesis performed in the sky plane. The multi-frequency 17 GHz to 39 GHz mosaics reveal spectral variations in the cm-wavelength continuum. At ∼30 arcsec resolutions, the 17-20 GHz intensities follow tightly the mid-IR, Icm∝I(8 μm), despite the breakdown of this correlation on larger scales. However, while the 33-39 GHz filament is parallel to IRAC 8 μm, it is offset by 15–20 arcsec towards the UV source. Such morphological differences in frequency reflect spectral variations, which we quantify spectroscopically as a sharp and steepening high-frequency cutoff, interpreted in terms of the spinning dust emission mechanism as a minimum grain size acutoff ∼ 6 ± 1 Å that increases deeper into the PDR.


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