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Related papers: Herschel SPIRE FTS Spectral Mapping Calibration

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A systematic programme of calibration observations was carried out to monitor the performance of the SPIRE FTS instrument on board the Herschel Space Observatory. Observations of planets (including the prime point-source calibrator,…

The Herschel SPIRE instrument consists of an imaging photometric camera and an imaging Fourier Transform Spectrometer (FTS), both operating over a frequency range of 450-1550 GHz. In this paper, we briefly review the FTS design, operation,…

The Fourier Transform Spectrometer (FTS) of the Spectral and Photometric Imaging REceiver (SPIRE) on board the ESA Herschel Space Observatory has two detector setting modes: (a) a nominal mode, which is optimized for observing moderately…

We provide a detailed description of the Herschel-SPIRE Fourier Transform Spectrometer (FTS) Spectral Feature Finder (FF). The FF is an automated process designed to extract significant spectral features from SPIRE FTS data products.…

Instrumentation and Methods for Astrophysics · Physics 2020-06-24 R. Hopwood , I. Valtchanov , Locke D. Spencer , J. P. Scott , C. S. Benson , N. Marchili , N. Hladczuk , E. T. Polehampton , N. Lu , G. Makiwa , D. A. Naylor , B. G. Gom , G. Noble , M. J. Griffin

The SPIRE Fourier Transform Spectrometer on board the Herschel Space Observatory had two standard spectral resolution modes for science observations: high resolution (HR) and low resolution (LR), which could also be performed in sequence…

Instrumentation and Methods for Astrophysics · Physics 2016-11-23 N. Marchili , R. Hopwood , T. Fulton , E. T. Polehampton , I. Valtchanov , J. Zaretski , D. A. Naylor , M. J. Griffin , P. Imhof , T. Lim , N. Lu , G. Makiwa , C. Pearson , L. Spencer

The Spectral and Photometric Imaging Receiver (SPIRE), is the Herschel Space Observatory`s submillimetre camera and spectrometer. It contains a three-band imaging photometer operating at 250, 350 and 500 microns, and an imaging Fourier…

Instrumentation and Methods for Astrophysics · Physics 2015-05-19 M. J. Griffin , A. Abergel , A. Abreu , P. A. R. Ade , P. André , J. -L. Augueres , T. Babbedge , Y. Bae , T. Baillie , J. -P. Baluteau , M. J. Barlow , G. Bendo , D. Benielli , J. J. Bock , P. Bonhomme , D. Brisbin , C. Brockley-Blatt , M. Caldwell , C. Cara , N. Castro-Rodriguez , R. Cerulli , P. Chanial , S. Chen , E. Clark , D. L. Clements , L. Clerc , J. Coker , D. Communal , L. Conversi , P. Cox , D. Crumb , C. Cunningham , F. Daly , G. R. Davis , P. De Antoni , J. Delderfield , N. Devin , A. Di Giorgio , I. Didschuns , K. Dohlen , M. Donati , A. Dowell , C. D. Dowell , L. Duband , L. Dumaye , R. J. Emery , M. Ferlet , D. Ferrand , J. Fontignie , M. Fox , A. Franceschini , M. Frerking , T. Fulton , J. Garcia , R. Gastaud , W. K. Gear , J. Glenn , A. Goizel , D. K. Griffin , T. Grundy , S. Guest , L. Guillemet , P. C. Hargrave , M. Harwit , P. Hastings , E. Hatziminaoglou , M. Herman , B. Hinde , V. Hristov , M. Huang , P. Imhof , K. J. Isaak , U. Israelsson , R. J. Ivison , D. Jennings , B. Kiernan , K. J. King , A. E. Lange , W. Latter , G. Laurent , P. Laurent , S. J. Leeks , E. Lellouch , L. Levenson , B. Li , J. Li , J. Lilienthal , T. Lim , J. Liu , N. Lu , S. Madden , G. Mainetti , P. Marliani , D. McKay , K. Mercier , S. Molinari , H. Morris , H. Moseley , J. Mulder , M. Mur , D. A. Naylor , H. Nguyen , B. O'Halloran , S. Oliver , G. Olofsson , H. -G. Olofsson , R. Orfei , M. J. Page , I. Pain , P. Panuzzo , A. Papageorgiou , G. Parks , P. Parr-Burman , A. Pearce , C. Pearson , I. Pérez-Fournon , F. Pinsard , G. Pisano , J. Podosek , M. Pohlen , E. T. Polehampton , D. Pouliquen , D. Rigopoulou , D. Rizzo , I. G. Roseboom , H. Roussel , M. Rowan-Robinson , B. Rownd , P. Saraceno , M. Sauvage , R. Savage , G. Savini , E. Sawyer , C. Scharmberg , D. Schmitt , N. Schneider , B. Schulz , A. Schwartz , R. Shafer , D. L. Shupe , B. Sibthorpe , S. Sidher , A. Smith , A. J. Smith , D. Smith , L. Spencer , B. Stobie , R. Sudiwala , K. Sukhatme , C. Surace , J. A. Stevens , B. M. Swinyard , M. Trichas , T. Tourette , H. Triou , S. Tseng , C. Tucker , A. Turner , M. Vaccari , I. Valtchanov , L. Vigroux , E. Virique , G. Voellmer , H. Walker , R. Ward , T. Waskett , M. Weilert , R. Wesson , G. J. White , N. Whitehouse , C. D. Wilson , B. Winter , A. L. Woodcraft , G. S. Wright , C. K. Xu , A. Zavagno , M. Zemcov , L. Zhang , E. Zonca

Herschel/SPIRE Fourier transform spectrometer (FTS) observations contain emission from both the Herschel Telescope and the SPIRE Instrument itself, both of which are typically orders of magnitude greater than the emission from the…

SPIRE, the Spectral and Photometric Imaging Receiver, is the Herschel Space Observatory's submillimetre camera and spectrometer. It contains a three-band imaging photometer operating at 250, 350 and 500 {\mu}m, and an imaging Fourier…

We describe an update to the Herschel-SPIRE Fourier-Transform Spectrometer (FTS) calibration for extended sources, which incorporates a correction for the frequency-dependent far-field feedhorn efficiency, $\eta_\mathrm{FF}$. This…

The SPIRE FTS Spectral Feature Finder (FF), developed within the Herschel Spectral and Photometric Imaging Receiver (SPIRE) Fourier Transform Spectrometer (FTS) instrument team, is an automated spectral feature fitting routine that attempts…

Instrumentation and Methods for Astrophysics · Physics 2020-06-24 Jeremy P. Scott , Locke D. Spencer , Rosalind Hopwood , Ivan Valtchanov , David A. Naylor

The Herschel SPIRE FTS Spectral Feature Finder (FF) detects significant spectral features within SPIRE spectra and employs two routines, and external references, to estimate source radial velocity. The first routine is based on the…

Instrumentation and Methods for Astrophysics · Physics 2020-06-24 Jeremy P. Scott , Natalia Hladczuk , Locke D. Spencer , Ivan Valtchanov , Chris S. Benson , Rosalind Hopwood

The ESA Herschel Spectral and Photometric Imaging Receiver (SPIRE) Fourier Transform Spectrometer (FTS) Spectral Feature Finder (FF) project is an automated spectral feature fitting routine developed within the SPIRE instrument team to…

Instrumentation and Methods for Astrophysics · Physics 2020-09-29 Chris S. Benson , N. Hladczuk , Locke D. Spencer , A. Robb , J. P. Scott , I. Valtchanov , R. Hopwood , David A. Naylor

The Spectral and Photometric Imaging Receiver (SPIRE) on the European Space Agency's Herschel Space Observatory utilizes a pioneering design for its imaging spectrometer in the form of a Fourier Transform Spectrometer (FTS). The standard…

The principles and practice of astronomical imaging Fourier transform spectroscopy (FTS) at far-infrared wavelengths are described. The Mach-Zehnder interferometer design has been widely adopted for current and future imaging FTS…

Instrumentation and Methods for Astrophysics · Physics 2013-10-10 David A. Naylor , Brad G. Gom , Matthijs H. D. van der Wiel , Gibion Makiwa

Emission from the Herschel telescope is the dominant source of radiation for the majority of SPIRE Fourier transform spectrometer (FTS) observations, despite the exceptionally low emissivity of the primary and secondary mirrors. Accurate…

The ESA Herschel Spectral and Photometric Imaging Receiver (SPIRE) Fourier Transform Spectrometer (FTS) Spectral Feature Finder (FF) project is an automated spectral feature fitting routine developed within the SPIRE instrument team to…

Astrophysics of Galaxies · Physics 2020-11-18 Chris S. Benson , L. D. Spencer , I. Valtchanov , J. Scott , N. Hładczuk

We present a method to derive the relative pointing offsets for SPIRE Fourier-Transform Spectrometer (FTS) solar system object (SSO) calibration targets, which were observed regularly throughout the Herschel mission. We construct ratios of…

The Far-Infrared Surveyor (FIS) onboard the AKARI satellite has a spectroscopic capability provided by a Fourier transform spectrometer (FIS-FTS). FIS-FTS is the first space-borne imaging FTS dedicated to far-infrared astronomical…

Photometric instruments operating at far infrared to millimetre wavelengths often have broad spectral passbands (central wavelength/bandwidth ~ 3 or less), especially those operating in space. A broad passband can result in significant…

We have obtained the first continuous disk averaged spectrum of Mars from 450 to 1550 Ghz using the Herschel-SPIRE Fourier Transform Spectrometer. The spectrum was obtained at a constant resolution of 1.4 GHz across the whole band. The flux…

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