Examinando por Autor "Vandenbussche, B."

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Calibration strategy for the SPICA/SAFARI instrument
(SPIE Digital Library, 2020-12-13) Shipman, R. F.; Vandenbussche, B.; Castillo Domínguez, E.; Labiano, Á.; Jellema, W.; Orlando, A.; Comunidad de Madrid; Angiola, O. [0000-0001-9464-3100]; info:eu-repo/semantics/restrictedAccess
SPICA is a mid to far infra-red space mission to explore the processes that form galaxies, stars and planets. SPICA/SAFARI is the far infrared spectrometer that provides near-background limited observations between 34 and 230 micrometers. The core of SAFARI consists of 4 grating modules, dispersing light onto 5 arrays of TES detectors per module. The grating modules provide low resolution (250) instantaneous spectra over the entire wavelength range. The high resolution (1500 to 12000) mode is accomplished by placing a Fourier Transform Spectrometer (FTS) in front of the gratings. Each grating module detector sees an interferogram from which the high resolution spectrum can be constructed. SAFARI data will be a convolution of complex spectral, temporal and spatial information. Along with spectral calibration accuracy of < 1 %, a relative flux calibration of 1% and an absolute flux calibration accuracy of 10% are required. This paper will discuss the calibration strategy and its impact on the instrument design of SAFARI
Acceso Abierto
The EChO science case
(Springer Link, 2015-11-29) Tinetti, G.; Drossart, P.; Eccleston, P.; Hartogh, P.; Isaak, K.; Linder, M.; Lovis, C.; Micela, G.; Olliver, M.; Puig, L.; Ribas, I.; Schrader, J. R.; Scholz, A.; Watkins, C.; Maillard, J. P.; Abreu, M.; Glasse, A.; Testi, L.; Doel, P.; Magnes, W.; Licandro Goldaracena, J.; Wawer, P.; Zapatero Osorio, M. R.; Decin, L.; Sánz Forcada, J.; Vakili, F.; Aylward, A.; Swain, M.; Sozzetti, A.; Filacchione, G.; Delgado Mena, E.; Read, P.; Lognonné, P.; Irshad, R.; Coates, A.; Cecchi Pestellini, C.; Thrastarson, H.; Brown, L.; Guillot, T.; Strazzulla, G.; Barstow, J. K.; Budaj, J.; Morgante, G.; Pietrzak, R.; Leconte, J.; Hersant, F.; De Sio, A.; Grassi, D.; Selsis, F.; Jarchow, C.; Fouqué, P.; Del Vecchio, C.; Tennyson, J.; Cassan, A.; Fernández Hernández, Maite; Burleigh, M. R.; Cordier, D.; De Witt, J.; Pagano, I.; Ray, T.; Gambicorti, L.; Palla, F.; Maldonado, J.; Biondi, D.; Eiroa, C.; Winek, W.; Ade, P.; Villaver, E.; Temple, J.; Gear, W.; Thompson, S.; Dominic, C.; Galand, M.; Focardi, M.; Cockell, C.; Pace, E.; Dorfi, E.; Bryson, I.; Cavarroc, C.; Pilat Lohinger, E.; Smith, A.; Eymet, V.; MacTavish, C.; Morales, J. C.; Gómez, H.; Stamper, R.; Esposito, M.; Andersen, A.; Azzollini, R.; Maxted, P.; Allende Prieto, C.; Nelson, R.; Gillon, M.; Achilleos, N.; Buchhave, L. A.; Fabrizio, N.; Ciaravella, A.; Claudi, R.; Damasso, M.; Bordé, P.; Figueira, P.; Rickman, H.; Rees, J. M.; Sitek, P.; Fossey, S.; Bakos, G.; Pascale, E.; Laken, B.; Soret, L.; Femenía Castella, B.; Allard, F.; Amado, P. J.; Luzzi, D.; Colomé, J.; Galand, M.; Lammer, H.; Bonford, B.; López Valverde, M. A.; Kerins, E.; Yung, Y.; Espinoza Contreras, M.; Irwin, P.; Herrero, E.; Wright, G.; Guàrdia, J.; Banaszkiewicz, M.; Hoogeeven, R.; Alcala, J.; Guio, P.; Koskinen, T.; Barton, E. J.; Piskunov, N.; Maurin, A. S.; Leto, G.; Boisse, I.; Claret, A.; Massi, F.; Kervella, P.; Börne, P.; Heiter, U.; Hargrave, P.; Fletcher, L.; Sánchez Béjar, V. J.; Bézard, B.; Cabral, A.; Michaut, C.; Winter, B.; Sousa, S.; Giuranna, M.; Batista, V.; Frith, J.; Ballerini, P.; López Morales, M.; Monteiro, M.; Tingley, B. W.; Lanza, N.; Maggio, A.; Lundgaard Rasmussen, I.; Altieri, F.; Covino, E.; Coustenis, A.; Heredero, R. L.; Watson, D.; Coudé du Foresto, V.; Liu, S. J.; Sicardy, B.; Deeg, H. J.; Moses, J.; Rodler, F.; Lithgow Bertelloni, C.; Demangeon, O.; Adybekian, V.; Fletcher, L.; Swinyard, B.; Morales Calderón, M.; Fouqué, P.; Deroo, P.; Lo Cicero, Ugo; Hueso, R.; Iro, N.; González Merino, B.; López Puertas, M.; Capria, M. T.; Danielski, C.; Branduardi Raymont, G.; Luntzer, A.; Gaulme, P.; Bulgarelli, A.; Parmentier, V.; Gerard, J. C.; Alard, C.; Frith, J.; Dobrijévic, M.; Medvedev, A.; Barrado, D.; Jacquemoud, S.; Sethenadh, J.; Readorn, K.; Polichtchouk, I.; Petrov, R.; García Piquer, A.; Tabernero, H. M.; White, G.; Pancrazzi, M.; García López, Ramón; Filacchione, G.; Gómez Leal, I.; Rengel, M.; Gesa, L.; Tanga, P.; Mueller Wodarg, I.; Israelian, G.; Rebolo López, R.; Shore, S.; Peralta, J.; Collura, A.; Giro, E.; Del Val Borro, M.; Griffith, C.; Tecsa, M.; Haigh, J.; Moro Martín, A.; Jones, H.; Gizon, L.; Pezzuto, S.; Giani, E.; Mall, U.; Eales, S.; Graczyk, R.; Ramos Zapata, G.; Krupp, N.; Sánchez Lavega, A.; Fossey, S.; Alonso Floriano, F. J.; Justtanot, K.; Santos, N.; Pérez Hoyos, S.; Savini, G.; Chamberlain, S.; Bowles, N.; Kerschbaum, F.; Tozzi, A.; Turrini, D.; Kipping, D.; Maruquette, J. B.; Correira, A.; Trifoglio, M.; Agúndez, Marcelino; Scandaratio, G.; Snellen, I. A.; Scuderi, S.; Femenía Castella, B.; Prisinzano, L.; Oliva, E.; Hébrard, E.; Lodieu, N.; Forget, F.; Chadney, J.; Showman, A.; Gustin, J.; Vinatier, S.; Charnoz, S.; Affer, L.; Rank Lüftinger, T.; Poretti, E.; Lahav, O.; North, C.; Gerard, J. C.; Murgas Alcaino, F.; Yurchenko, S. N.; Widemann, T.; Ward Thompson, D.; Montañés Rodríguez, P.; Kovács, G.; Valdivieso, M. L.; Moya Bedon, A.; Montalto, M.; Christian Jessen, N.; Venot, O.; Koskinen, T.; Lagage, P. O.; Bellucci, G.; Prinja, R.; Pinfield, D.; Banaszkiewicz, M.; Waldmann, I.; Jones, G.; Morello, G.; Crook, J.; Lim, T.; Parviainen, H.; Pallé, E.; Ramos, A. A.; Sanromá, E.; Waters, R.; Morais, H.; Stiepen, A.; Lellouch, E.; Orton, G.; Rezac, L.; Beaulieu, J. P.; Focardi, M.; Mauskopf, P.; Barlow, M.; Guedel, M.; Waltham, D.; Agnor, C.; Encrenaz, T.; Cerulli, R.; Balado, A.; Bouy, H.; Rebordao, J.; Stolarski, M.; Álvarez Iglesias, C. A.; Adriani, A.; Rocchetto, M.; Norgaard Nielsen, H. U.; Hollis, M.; Selig, A.; Malaguti, G.; Burston, R.; Peña Ramírez, K. Y.; Schmider, F. X.; Baffa, C.; Heyrovsky, D.; Figueira, P.; Piccioni, G.; Ottensamer, R.; Radioti, A.; Yelle, R.; Pantin, E.; Miles Paez, P.; Belmonte Avilés, J. A.; Montes, D.; Varley, R.; Viti, S.; Abe, L.; Pinsard, F.; Tessenyi, M.; Di Giorgio, A.; Turrini, D.; Terenzi, L.; Hubert, B.; Griffin, M.; Barber, R. J.; Cole, R.; Gianotti, F.; Blecka, M.; Wawrzaszk, A.; Middleton, K.; De Kok, R.; Martín Torres, Javier; Kehoe, T.; Cho, J.; Machado, P.; Berry, D.; Wisniowski, T.; Grodent, D.; Rataj, M.; Hornstrup, A.; Kerschbaum, F.; Vandenbussche, B.; Stixrude, L.; González Hernández, Carmen; Rebordao, J. [0000-0002-7418-0345]; Kerschbaum, F. [0000-0001-6320-0980]; Abreu, M. [0000-0002-0716-9568]; Tabernero, H. [0000-0002-8087-4298]; López Puertas, M. [0000-0003-2941-7734]; Jacquemoud, S. [0000-0002-1500-5256]; Tennyson, J. [0000-0002-4994-5238]; Focardi, M. [0000-0002-3806-4283]; Leto, G. [0000-0002-0040-5011]; Lodieu, N. [0000-0002-3612-8968]; Tinetti, G. [0000-0001-6058-6654]; Bulgarelli, A. [0000-0001-6347-0649]; Morales Calderon, M. [0000-0001-9526-9499]; Ward Thompson, D. [0000-0003-1140-2761]; Rebolo, R. [0000-0003-3767-7085]; López Valverde, M. A. [0000-0002-7989-4267]; Gillon, M. [0000-0003-1462-7739]; Morgante, G. [0000-0001-9234-7412]; Pena Ramírez, K. [0000-0002-5855-401X]; Galand, M. [0000-0001-5797-914X]; Pancrazzi, M. [0000-0002-3789-2482]; Pilat Lohinger, E. [0000-0002-5292-1923]; Altieri, F. [0000-0002-6338-8300]; Malaguti, G. [0000-0001-9872-3378]; Sánchez Lavega, A. [0000-0001-7234-7634]; Waldmann, I. [0000-0002-4205-5267]; Kovacs, G. [0000-0002-2365-2330]; Guillot, T. [0000-0002-7188-8428]; Monteiro, M. [0000-0001-5644-0898]; Bellucci, G. [0000-0003-0867-8679]; Baffa, C. [0000-0002-4935-100X]; Olivia, E. [0000-0002-9123-0412]; Tizzi, A. [0000-0002-6725-3825]; Selsis, F. [0000-0001-9619-5356]; Scuderi, Salvatore [0000-0002-8637-2109]; Hersant, F. [0000-0002-2687-7500]; Gear, W. [0000-0001-6789-6196]; Damasso, M. [0000-0001-9984-4278]; Irwin, P. [0000-0002-6772-384X]; Pinfield, D. [0000-0002-7804-4260]; Kipping, D. [0000-0002-4365-7366]; Maldonado, J. [0000-0002-4282-1072]; Pace, E. [0000-0001-5870-1772]; Burleigh, M. [0000-0003-0684-7803]; Chadney, J. [0000-0002-5174-2114]; Moro Martín, A. [0000-0001-9504-8426]; Claret, A. [0000-0002-4045-8134]; Rodríguez, P. [0000-0002-6855-9682]; Bezard, B. [0000-0002-5433-5661]; Gómez, H. [0000-0003-3398-0052]; Maldonado, J. [0000-0002-2218-5689]; Michaut, C. [0000-0002-2578-0117]; Hornstrup, A. [0000-0002-3363-0936]; Scholz, A. [0000-0001-8993-5053]; Sánchez Bejar, V. [0000-0002-5086-4232]; López Heredero, R. [0000-0002-2197-8388]; Sanz Forcada, J. [0000-0002-1600-7835]; Danielski, C. [0000-0002-3729-2663]; Vandenbussche, B. [0000-0002-1368-3109]; Sousa, S. [0000-0001-9047-2965]; Medved, A. [0000-0003-2713-8977]; Tinetti, G. [0000-0001-6058-6654]; Bakos, G. [0000-0001-7204-6727]; Ade, P. [0000-0002-5127-0401]; Amado, P. J. [0000-0002-8388-6040]; Martín Torres, J. [0000-0001-6479-2236]; Correira, A. [0000-0002-8946-8579]; Haigh, J. [0000-0001-5504-4754]; Scandariato, G. [0000-0003-2029-0626]; Guedel, M. [0000-0001-9818-0588]; Piskunov, N. [0000-0001-5742-7767]; Adibekyan, V. [0000-0002-0601-6199]; Pérez Hoyos, S. [0000-0001-9797-4917]; Poretti, E. [0000-0003-1200-0473]; Maggio, A. [0000-0001-5154-6108]; Kervella, P. [0000-0003-0626-1749]; Pascale, E. [0000-0002-3242-8154]; Claudi, R. [0000-0001-7707-5105]; Filacchione, G. [0000-0001-9567-0055]; Rickman, H. [0000-0002-9603-6619]; Sanroma, E. [0000-0001-8859-7937]; Agundez, M. [0000-0003-3248-3564]; Montes, D. [0000-0002-7779-238X]; Fletcher, L. [0000-0001-5834-9588]; Rataj, M. [0000-0002-2978-9629]; Stixrude, L. [0000-0003-3778-2432]; Montes, D. [0000-0002-7779-238X]; Morais, M. H. [0000-0001-5333-2736]; Hueso, R. [0000-0003-0169-123X]; Yurchenko, S. [0000-0001-9286-9501]; Morales, J. C. [0000-0003-0061-518X]; Pérez Hoyos, S. [0000-0002-2587-4682]; Santos, N. [0000-0003-4422-2919]; Peralta, J. [0000-0002-6823-1695]; Budaj, J. [0000-0002-9125-7340]; Barlow, M. [0000-0002-3875-1171]; Deeg, H. [0000-0003-0047-4241]; Grassi, D. [0000-0003-1653-3066]; Piccioni, G. [0000-0002-7893-6808]; Barton, E. [0000-0001-5945-9244]; Abreu, M. [0000-0002-0716-9568]; Ribas, I. [0000-0002-6689-0312]; Coates, A. [0000-0002-6185-3125]; García Ramón, J. [0000-0002-8204-6832]; Bouy, H. [0000-0002-7084-487X[; Lognonne, P. [0000-0002-1014-920X]; Demangeon, O. [0000-0001-7918-0355]; Ray, T. [0000-0002-2110-1068]; Guio, P. [0000-0002-1607-5862]; Tanga, P. [0000-0002-2718-997X]; Delgado, M. E. [0000-0003-4434-2195]; Leto, G. [0000-0002-0040-5011]; Prisinzano, L. [0000-0002-8893-2210]; Barstow, J. [0000-0003-3726-5419]; Balado, A. [0000-0003-4268-2516]; Lithgow Bertelloni, C. [0000-0003-0924-6587]; Zapatero Osorio, M. R. [0000-0001-5664-2852]; Affer, L. [0000-0001-5600-3778]; Ciaravella, A. [0000-0002-3127-8078]; Barrado Navascues, D. [0000-0002-5971-9242]; Figueira, P. [0000-0001-8504-283X]; Covino, E. [0000-0002-6187-6685]; Venot, O. [0000-0003-2854-765X]; Cabral, A. [0000-0002-9433-871X]; Watson, D. [0000-0002-4465-8264]; Turrini, D. [0000-0002-1923-7740]
The discovery of almost two thousand exoplanets has revealed an unexpectedly diverse planet population. We see gas giants in few-day orbits, whole multi-planet systems within the orbit of Mercury, and new populations of planets with masses between that of the Earth and Neptune—all unknown in the Solar System. Observations to date have shown that our Solar System is certainly not representative of the general population of planets in our Milky Way. The key science questions that urgently need addressing are therefore: What are exoplanets made of? Why are planets as they are? How do planetary systems work and what causes the exceptional diversity observed as compared to the Solar System? The EChO (Exoplanet Characterisation Observatory) space mission was conceived to take up the challenge to explain this diversity in terms of formation, evolution, internal structure and planet and atmospheric composition. This requires in-depth spectroscopic knowledge of the atmospheres of a large and well-defined planet sample for which precise physical, chemical and dynamical information can be obtained. In order to fulfil this ambitious scientific program, EChO was designed as a dedicated survey mission for transit and eclipse spectroscopy capable of observing a large, diverse and well-defined planet sample within its 4-year mission lifetime. The transit and eclipse spectroscopy method, whereby the signal from the star and planet are differentiated using knowledge of the planetary ephemerides, allows us to measure atmospheric signals from the planet at levels of at least 10−4 relative to the star. This can only be achieved in conjunction with a carefully designed stable payload and satellite platform. It is also necessary to provide broad instantaneous wavelength coverage to detect as many molecular species as possible, to probe the thermal structure of the planetary atmospheres and to correct for the contaminating effects of the stellar photosphere. This requires wavelength coverage of at least 0.55 to 11 μm with a goal of covering from 0.4 to 16 μm. Only modest spectral resolving power is needed, with R ~ 300 for wavelengths less than 5 μm and R ~ 30 for wavelengths greater than this. The transit spectroscopy technique means that no spatial resolution is required. A telescope collecting area of about 1 m2 is sufficiently large to achieve the necessary spectro-photometric precision: for the Phase A study a 1.13 m2 telescope, diffraction limited at 3 μm has been adopted. Placing the satellite at L2 provides a cold and stable thermal environment as well as a large field of regard to allow efficient time-critical observation of targets randomly distributed over the sky. EChO has been conceived to achieve a single goal: exoplanet spectroscopy. The spectral coverage and signal-to-noise to be achieved by EChO, thanks to its high stability and dedicated design, would be a game changer by allowing atmospheric composition to be measured with unparalleled exactness: at least a factor 10 more precise and a factor 10 to 1000 more accurate than current observations. This would enable the detection of molecular abundances three orders of magnitude lower than currently possible and a fourfold increase from the handful of molecules detected to date. Combining these data with estimates of planetary bulk compositions from accurate measurements of their radii and masses would allow degeneracies associated with planetary interior modelling to be broken, giving unique insight into the interior structure and elemental abundances of these alien worlds. EChO would allow scientists to study exoplanets both as a population and as individuals. The mission can target super-Earths, Neptune-like, and Jupiter-like planets, in the very hot to temperate zones (planet temperatures of 300–3000 K) of F to M-type host stars. The EChO core science would be delivered by a three-tier survey. The EChO Chemical Census: This is a broad survey of a few-hundred exoplanets, which allows us to explore the spectroscopic and chemical diversity of the exoplanet population as a whole. The EChO Origin: This is a deep survey of a subsample of tens of exoplanets for which significantly higher signal to noise and spectral resolution spectra can be obtained to explain the origin of the exoplanet diversity (such as formation mechanisms, chemical processes, atmospheric escape). The EChO Rosetta Stones: This is an ultra-high accuracy survey targeting a subsample of select exoplanets. These will be the bright “benchmark” cases for which a large number of measurements would be taken to explore temporal variations, and to obtain two and three dimensional spatial information on the atmospheric conditions through eclipse-mapping techniques. If EChO were launched today, the exoplanets currently observed are sufficient to provide a large and diverse sample. The Chemical Census survey would consist of > 160 exoplanets with a range of planetary sizes, temperatures, orbital parameters and stellar host properties. Additionally, over the next 10 years, several new ground- and space-based transit photometric surveys and missions will come on-line (e.g. NGTS, CHEOPS, TESS, PLATO), which will specifically focus on finding bright, nearby systems. The current rapid rate of discovery would allow the target list to be further optimised in the years prior to EChO’s launch and enable the atmospheric characterisation of hundreds of planets.
Acceso Abierto
The nature of point source fringes in mid-infrared spectra acquired with the James Webb Space Telescope
(EDP Sciences, 2020-09-23) Argyriou, I.; Wells, M.; Glasse, A.; Lee, D.; Royer, P.; Vandenbussche, B.; Malamuth, E.; Glauser, A.; Kavanagh, P. J.; Labiano, Á.; Lahuis, F.; Mueller, M.; Patapis, P.; Comunidad de Madrid; Argyriou, I. [0000-0003-2820-1077]; Patapis, P. [0000-0001-8718-3732]; Unidad de Excelencia Científica María de Maeztu Centro de Astrobiología del Instituto Nacional de Técnica Aeroespacial y CSIC, MDM-2017-0737
Context. As is common for infrared spectrometers, the constructive and destructive interference in different layers of the James Webb Space Telescope (JWST) Mid-Infrared Instrument (MIRI) detector arrays modulate the detected signal as a function of wavelength. The resulting “fringing” in the Medium-Resolution Spectrometer (MRS) spectra varies in amplitude between 10% and 30% of the spectral baseline. A common method for correcting for fringes relies on dividing the data by a fringe flat. In the case of MIRI MRS, the fringe flat is derived from measurements of an extended, spatially homogeneous source acquired during the thermal-vacuum ground verification of the instrument. While this approach reduces fringe amplitudes of extended sources below the percent level, at the detector level, point source fringe residuals vary in a systematic way across the point spread function. The effect could hamper the scientific interpretation of MRS observations of unresolved sources, semi-extended sources, and point sources in crowded fields. Aims. We find MIRI MRS point source fringes to be reproducible under similar observing conditions. We want to investigate whether a generic and accurate correction can be determined. Therefore, we want to identify the variables, if they exist, that would allow for a parametrization of the signal variations induced by point source fringe modulations. Methods. We determine the point source fringe properties by analyzing MRS detector plane images acquired on the ground. We extracted the fringe profile of multiple point source observations and studied the amplitude and phase of the fringes as a function of field position and pixel sampling of the point spread function of the optical chain. Results. A systematic variation in the amplitude and phase of the point source fringes is found over the wavelength range covered by the test sources (4.9 − 5.8 μm). The variation depends on the fraction of the point spread function seen by the detector pixel. We identify the non-uniform pixel illumination as the root cause of the reported systematic variation. This new finding allows us to reconcile the point source and extended source fringe patterns observed in test data during ground verification. We report an improvement after correction of 50% on the 1σ standard deviation of the spectral continuum. A 50% improvement is also reported in line sensitivity for a benchmark test with a spectral continuum of 100 mJy. The improvement in the shape of weak lines is illustrated using a T Tauri model spectrum. Consequently, we verify that fringes of extended sources and potentially semi-extended sources and crowded fields can be simulated by combining multiple point source fringe transmissions. Furthermore, we discuss the applicability of this novel fringe-correction method to the MRS data (and the data of other instruments).