100 results on '"Luciano Gottardi"'
Search Results
2. The Athena X-ray Integral Field Unit: a consolidated design for the system requirement review of the preliminary definition phase
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Didier Barret, Vincent Albouys, Jan-Willem den Herder, Luigi Piro, Massimo Cappi, Juhani Huovelin, Richard Kelley, J. Miguel Mas-Hesse, Stéphane Paltani, Gregor Rauw, Agata Rozanska, Jiri Svoboda, Joern Wilms, Noriko Yamasaki, Marc Audard, Simon Bandler, Marco Barbera, Xavier Barcons, Enrico Bozzo, Maria Teresa Ceballos, Ivan Charles, Elisa Costantini, Thomas Dauser, Anne Decourchelle, Lionel Duband, Jean-Marc Duval, Fabrizio Fiore, Flavio Gatti, Andrea Goldwurm, Roland den Hartog, Brian Jackson, Peter Jonker, Caroline Kilbourne, Seppo Korpela, Claudio Macculi, Mariano Mendez, Kazuhisa Mitsuda, Silvano Molendi, François Pajot, Etienne Pointecouteau, Frederick Porter, Gabriel W. Pratt, Damien Prêle, Laurent Ravera, Kosuke Sato, Joop Schaye, Keisuke Shinozaki, Konrad Skup, Jan Soucek, Tanguy Thibert, Jacco Vink, Natalie Webb, Laurence Chaoul, Desi Raulin, Aurora Simionescu, Jose Miguel Torrejon, Fabio Acero, Graziella Branduardi-Raymont, Stefano Ettori, Alexis Finoguenov, Nicolas Grosso, Jelle Kaastra, Pasquale Mazzotta, Jon Miller, Giovanni Miniutti, Fabrizio Nicastro, Salvatore Sciortino, Hiroya Yamaguchi, Sophie Beaumont, Edoardo Cucchetti, Matteo D’Andrea, Megan Eckart, Philippe Ferrando, Elias Kammoun, Simone Lotti, Jean-Michel Mesnager, Lorenzo Natalucci, Philippe Peille, Jelle de Plaa, Florence Ardellier, Andrea Argan, Elise Bellouard, Jérôme Carron, Elisabetta Cavazzuti, Mauro Fiorini, Pourya Khosropanah, Sylvain Martin, James Perry, Frederic Pinsard, Alice Pradines, Manuela Rigano, Peter Roelfsema, Denis Schwander, Guido Torrioli, Joel Ullom, Isabel Vera, Eduardo Medinaceli Villegas, Monika Zuchniak, Frank Brachet, Ugo Lo Cicero, William Doriese, Malcom Durkin, Valentina Fioretti, Hervé Geoffray, Lionel Jacques, Christian Kirsch, Stephen Smith, Joseph Adams, Emilie Gloaguen, Ruud Hoogeveen, Paul van der Hulst, Mikko Kiviranta, Jan van der Kuur, Aurélien Ledot, Bert-Joost van Leeuwen, Dennis van Loon, Bertrand Lyautey, Yann Parot, Kazuhiro Sakai, Henk van Weers, Shariefa Abdoelkariem, Thomas Adam, Christophe Adami, Corinne Aicardi, Hiroki Akamatsu, Pablo Eleazar Merino Alonso, Roberta Amato, Jérôme André, Matteo Angelinelli, Manuel Anon-Cancela, Shebli Anvar, Ricardo Atienza, Anthony Attard, Natalia Auricchio, Ana Balado, Florian Bancel, Lorenzo Ferrari Barusso, Arturo Bascuñan, Vivian Bernard, Alicia Berrocal, Sylvie Blin, Donata Bonino, François Bonnet, Patrick Bonny, Peter Boorman, Charles Boreux, Ayoub Bounab, Martin Boutelier, Kevin Boyce, Daniele Brienza, Marcel Bruijn, Andrea Bulgarelli, Simona Calarco, Paul Callanan, Alberto Prada Campello, Thierry Camus, Florent Canourgues, Vito Capobianco, Nicolas Cardiel, Florent Castellani, Oscar Cheatom, James Chervenak, Fabio Chiarello, Laurent Clerc, Nicolas Clerc, Beatriz Cobo, Odile Coeur-Joly, Alexis Coleiro, Stéphane Colonges, Leonardo Corcione, Mickael Coriat, Alexandre Coynel, Francesco Cuttaia, Antonino D’Ai, Fabio D’anca, Mauro Dadina, Christophe Daniel, Lea Dauner, Natalie DeNigris, Johannes Dercksen, Michael DiPirro, Eric Doumayrou, Luc Dubbeldam, Michel Dupieux, Simon Dupourqué, Jean Louis Durand, Dominique Eckert, Valvanera Eiriz, Eric Ercolani, Christophe Etcheverry, Fred Finkbeiner, Mariateresa Fiocchi, Hervé Fossecave, Philippe Franssen, Martin Frericks, Stefano Gabici, Florent Gant, Jian-Rong Gao, Fabio Gastaldello, Ludovic Genolet, Simona Ghizzardi, Ma Angeles Alcacera Gil, Elisa Giovannini, Olivier Godet, Javier Gomez-Elvira, Raoul Gonzalez, Manuel Gonzalez, Luciano Gottardi, Dolorès Granat, Michel Gros, Nicolas Guignard, Paul Hieltjes, Adolfo Jesús Hurtado, Kent Irwin, Christian Jacquey, Agnieszka Janiuk, Jean Jaubert, Maria Jiménez, Antoine Jolly, Thierry Jourdan, Sabine Julien, Bartosz Kedziora, Andrew Korb, Ingo Kreykenbohm, Ole König, Mathieu Langer, Philippe Laudet, Philippe Laurent, Monica Laurenza, Jean Lesrel, Sebastiano Ligori, Maximilian Lorenz, Alfredo Luminari, Bruno Maffei, Océane Maisonnave, Lorenzo Marelli, Didier Massonet, Irwin Maussang, Alejandro Gonzalo Melchor, Isabelle Le Mer, Francisco Javier San Millan, Jean-Pierre Millerioux, Teresa Mineo, Gabriele Minervini, Alexeï Molin, David Monestes, Nicola Montinaro, Baptiste Mot, David Murat, Kenichiro Nagayoshi, Yaël Nazé, Loïc Noguès, Damien Pailot, Francesca Panessa, Luigi Parodi, Pascal Petit, Enrico Piconcelli, Ciro Pinto, Jose Miguel Encinas Plaza, Borja Plaza, David Poyatos, Thomas Prouvé, Andy Ptak, Simonetta Puccetti, Elena Puccio, Pascale Ramon, Manuel Reina, Guillaume Rioland, Louis Rodriguez, Anton Roig, Bertrand Rollet, Mauro Roncarelli, Gilles Roudil, Tomasz Rudnicki, Julien Sanisidro, Luisa Sciortino, Vitor Silva, Michael Sordet, Javier Soto-Aguilar, Pierre Spizzi, Christian Surace, Miguel Fernández Sánchez, Emanuele Taralli, Guilhem Terrasa, Régis Terrier, Michela Todaro, Pietro Ubertini, Michela Uslenghi, Jan Geralt Bij de Vaate, Davide Vaccaro, Salvatore Varisco, Peggy Varnière, Laurent Vibert, María Vidriales, Fabrizio Villa, Boris Martin Vodopivec, Angela Volpe, Cor de Vries, Nicholas Wakeham, Gavin Walmsley, Michael Wise, Martin de Wit, Grzegorz Woźniak, Barret, Didier, Albouys, Vincent, Herder, Jan-Willem den, Piro, Luigi, Cappi, Massimo, Huovelin, Juhani, Kelley, Richard, Mas-Hesse, J. Miguel, Paltani, Stéphane, Rauw, Gregor, Rozanska, Agata, Svoboda, Jiri, Wilms, Joern, Yamasaki, Noriko, Audard, Marc, Bandler, Simon, Barbera, Marco, Barcons, Xavier, Bozzo, Enrico, Ceballos, Maria Teresa, Charles, Ivan, Costantini, Elisa, Dauser, Thoma, Decourchelle, Anne, Duband, Lionel, Duval, Jean-Marc, Fiore, Fabrizio, Gatti, Flavio, Goldwurm, Andrea, Hartog, Roland den, Jackson, Brian, Jonker, Peter, Kilbourne, Caroline, Korpela, Seppo, Macculi, Claudio, Mendez, Mariano, Mitsuda, Kazuhisa, Molendi, Silvano, Pajot, Françoi, Pointecouteau, Etienne, Porter, Frederick, Pratt, Gabriel W., Prêle, Damien, Ravera, Laurent, Sato, Kosuke, Schaye, Joop, Shinozaki, Keisuke, Skup, Konrad, Soucek, Jan, Thibert, Tanguy, Vink, Jacco, Webb, Natalie, Chaoul, Laurence, Raulin, Desi, Simionescu, Aurora, Torrejon, Jose Miguel, Acero, Fabio, Branduardi-Raymont, Graziella, Ettori, Stefano, Finoguenov, Alexi, Grosso, Nicola, Kaastra, Jelle, Mazzotta, Pasquale, Miller, Jon, Miniutti, Giovanni, Nicastro, Fabrizio, Sciortino, Salvatore, Yamaguchi, Hiroya, Beaumont, Sophie, Cucchetti, Edoardo, D’Andrea, Matteo, Eckart, Megan, Ferrando, Philippe, Kammoun, Elia, Lotti, Simone, Mesnager, Jean-Michel, Natalucci, Lorenzo, Peille, Philippe, de Plaa, Jelle, Ardellier, Florence, Argan, Andrea, Bellouard, Elise, Carron, Jérôme, Cavazzuti, Elisabetta, Fiorini, Mauro, Khosropanah, Pourya, Martin, Sylvain, Perry, Jame, Pinsard, Frederic, Pradines, Alice, Rigano, Manuela, Roelfsema, Peter, Schwander, Deni, Torrioli, Guido, Ullom, Joel, Vera, Isabel, Villegas, Eduardo Medinaceli, Zuchniak, Monika, Brachet, Frank, Cicero, Ugo Lo, Doriese, William, Durkin, Malcom, Fioretti, Valentina, Geoffray, Hervé, Jacques, Lionel, Kirsch, Christian, Smith, Stephen, Adams, Joseph, Gloaguen, Emilie, Hoogeveen, Ruud, van der Hulst, Paul, Kiviranta, Mikko, van der Kuur, Jan, Ledot, Aurélien, van Leeuwen, Bert-Joost, van Loon, Denni, Lyautey, Bertrand, Parot, Yann, Sakai, Kazuhiro, van Weers, Henk, Abdoelkariem, Shariefa, Adam, Thoma, Adami, Christophe, Aicardi, Corinne, Akamatsu, Hiroki, Alonso, Pablo Eleazar Merino, Amato, Roberta, André, Jérôme, Angelinelli, Matteo, Anon-Cancela, Manuel, Anvar, Shebli, Atienza, Ricardo, Attard, Anthony, Auricchio, Natalia, Balado, Ana, Bancel, Florian, Barusso, Lorenzo Ferrari, Bascuñan, Arturo, Bernard, Vivian, Berrocal, Alicia, Blin, Sylvie, Bonino, Donata, Bonnet, Françoi, Bonny, Patrick, Boorman, Peter, Boreux, Charle, Bounab, Ayoub, Boutelier, Martin, Boyce, Kevin, Brienza, Daniele, Bruijn, Marcel, Bulgarelli, Andrea, Calarco, Simona, Callanan, Paul, Campello, Alberto Prada, Camus, Thierry, Canourgues, Florent, Capobianco, Vito, Cardiel, Nicola, Castellani, Florent, Cheatom, Oscar, Chervenak, Jame, Chiarello, Fabio, Clerc, Laurent, Clerc, Nicola, Cobo, Beatriz, Coeur-Joly, Odile, Coleiro, Alexi, Colonges, Stéphane, Corcione, Leonardo, Coriat, Mickael, Coynel, Alexandre, Cuttaia, Francesco, D’Ai, Antonino, D’anca, Fabio, Dadina, Mauro, Daniel, Christophe, Dauner, Lea, DeNigris, Natalie, Dercksen, Johanne, DiPirro, Michael, Doumayrou, Eric, Dubbeldam, Luc, Dupieux, Michel, Dupourqué, Simon, Durand, Jean Loui, Eckert, Dominique, Eiriz, Valvanera, Ercolani, Eric, Etcheverry, Christophe, Finkbeiner, Fred, Fiocchi, Mariateresa, Fossecave, Hervé, Franssen, Philippe, Frericks, Martin, Gabici, Stefano, Gant, Florent, Gao, Jian-Rong, Gastaldello, Fabio, Genolet, Ludovic, Ghizzardi, Simona, Gil, Ma Angeles Alcacera, Giovannini, Elisa, Godet, Olivier, Gomez-Elvira, Javier, Gonzalez, Raoul, Gonzalez, Manuel, Gottardi, Luciano, Granat, Dolorè, Gros, Michel, Guignard, Nicola, Hieltjes, Paul, Hurtado, Adolfo Jesú, Irwin, Kent, Jacquey, Christian, Janiuk, Agnieszka, Jaubert, Jean, Jiménez, Maria, Jolly, Antoine, Jourdan, Thierry, Julien, Sabine, Kedziora, Bartosz, Korb, Andrew, Kreykenbohm, Ingo, König, Ole, Langer, Mathieu, Laudet, Philippe, Laurent, Philippe, Laurenza, Monica, Lesrel, Jean, Ligori, Sebastiano, Lorenz, Maximilian, Luminari, Alfredo, Maffei, Bruno, Maisonnave, Océane, Marelli, Lorenzo, Massonet, Didier, Maussang, Irwin, Melchor, Alejandro Gonzalo, Le Mer, Isabelle, Millan, Francisco Javier San, Millerioux, Jean-Pierre, Mineo, Teresa, Minervini, Gabriele, Molin, Alexeï, Monestes, David, Montinaro, Nicola, Mot, Baptiste, Murat, David, Nagayoshi, Kenichiro, Nazé, Yaël, Noguès, Loïc, Pailot, Damien, Panessa, Francesca, Parodi, Luigi, Petit, Pascal, Piconcelli, Enrico, Pinto, Ciro, Plaza, Jose Miguel Encina, Plaza, Borja, Poyatos, David, Prouvé, Thoma, Ptak, Andy, Puccetti, Simonetta, Puccio, Elena, Ramon, Pascale, Reina, Manuel, Rioland, Guillaume, Rodriguez, Loui, Roig, Anton, Rollet, Bertrand, Roncarelli, Mauro, Roudil, Gille, Rudnicki, Tomasz, Sanisidro, Julien, Sciortino, Luisa, Silva, Vitor, Sordet, Michael, Soto-Aguilar, Javier, Spizzi, Pierre, Surace, Christian, Sánchez, Miguel Fernández, Taralli, Emanuele, Terrasa, Guilhem, Terrier, Régi, Todaro, Michela, Ubertini, Pietro, Uslenghi, Michela, de Vaate, Jan Geralt Bij, Vaccaro, Davide, Varisco, Salvatore, Varnière, Peggy, Vibert, Laurent, Vidriales, María, Villa, Fabrizio, Vodopivec, Boris Martin, Volpe, Angela, de Vries, Cor, Wakeham, Nichola, Walmsley, Gavin, Wise, Michael, de Wit, Martin, Woźniak, Grzegorz, Universidad de Alicante. Departamento de Física, Ingeniería de Sistemas y Teoría de la Señal, Universidad de Alicante. Instituto Universitario de Física Aplicada a las Ciencias y las Tecnologías, Astronomía y Astrofísica, Agencia Estatal de Investigación (AEI), Ministerio de Ciencia e Innovación (MICINN), Centre National D'Etudes Spatiales (CNES), Agenzia Spaziale Italiana (ASI), European Space Agency (ESA), Institut de recherche en astrophysique et planétologie (IRAP), Université Toulouse III - Paul Sabatier (UT3), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire Midi-Pyrénées (OMP), Institut de Recherche pour le Développement (IRD)-Université Toulouse III - Paul Sabatier (UT3), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Institut de Recherche pour le Développement (IRD)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Centre National de la Recherche Scientifique (CNRS), SRON Netherlands Institute for Space Research (SRON), Department of Physics [Helsinki], Falculty of Science [Helsinki], Helsingin yliopisto = Helsingfors universitet = University of Helsinki-Helsingin yliopisto = Helsingfors universitet = University of Helsinki, Institut d'Astrophysique et de Géophysique [Liège], Université de Liège, Centrum Astronomiczne im. M. Kopernika, Warszawa (CAMK), Faculty of Civil Engineering [Prague] (FSV CTU), Czech Technical University in Prague (CTU), Columbia Astrophysics Laboratory (CAL), Columbia University [New York], NASA Goddard Space Flight Center (GSFC), AstroParticule et Cosmologie (APC (UMR_7164)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPCité), Institut d'astrophysique spatiale (IAS), and Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Centre National d’Études Spatiales [Paris] (CNES)
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X-IFU: The X-ray Integral Field Unit ,Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,The X-ray Integral Field Unit [X-IFU] ,Solar and stellar astrophysics ,FOS: Physical sciences ,[PHYS.ASTR.CO]Physics [physics]/Astrophysics [astro-ph]/Cosmology and Extra-Galactic Astrophysics [astro-ph.CO] ,Settore FIS/05 - Astronomia E Astrofisica ,X-rays ,SDG 7 - Affordable and Clean Energy ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Solar and Stellar Astrophysics (astro-ph.SR) ,High Energy Astrophysical Phenomena (astro-ph.HE) ,Astrophysics of Galaxies ,Athena: the advanced telescope for high energy astrophysics ,Astronomy and Astrophysics ,Astrophysics - Astrophysics of Galaxies ,Astrophysical phenomena ,Space instrumentation ,Astrophysics - Solar and Stellar Astrophysics ,High energy ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,[PHYS.GRQC]Physics [physics]/General Relativity and Quantum Cosmology [gr-qc] ,the advanced telescope for high energy astrophysics [Athena] ,Athena: the advanced telescope for high energy astrophysics · X-IFU: The X-ray Integral Field Unit · Space instrumentation · X-rays · Observatory ,Observatory ,Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - High Energy Astrophysical Phenomena ,SDG 12 - Responsible Consumption and Production ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
The Athena X-ray Integral Unit (X-IFU) is the high resolution X-ray spectrometer, studied since 2015 for flying in the mid-30s on the Athena space X-ray Observatory, a versatile observatory designed to address the Hot and Energetic Universe science theme, selected in November 2013 by the Survey Science Committee. Based on a large format array of Transition Edge Sensors (TES), it aims to provide spatially resolved X-ray spectroscopy, with a spectral resolution of 2.5 eV (up to 7 keV) over an hexagonal field of view of 5 arc minutes (equivalent diameter). The X-IFU entered its System Requirement Review (SRR) in June 2022, at about the same time when ESA called for an overall X-IFU redesign (including the X-IFU cryostat and the cooling chain), due to an unanticipated cost overrun of Athena. In this paper, after illustrating the breakthrough capabilities of the X-IFU, we describe the instrument as presented at its SRR, browsing through all the subsystems and associated requirements. We then show the instrument budgets, with a particular emphasis on the anticipated budgets of some of its key performance parameters. Finally we briefly discuss on the ongoing key technology demonstration activities, the calibration and the activities foreseen in the X-IFU Instrument Science Center, and touch on communication and outreach activities, the consortium organisation, and finally on the life cycle assessment of X-IFU aiming at minimising the environmental footprint, associated with the development of the instrument. Thanks to the studies conducted so far on X-IFU, it is expected that along the design-to-cost exercise requested by ESA, the X-IFU will maintain flagship capabilities in spatially resolved high resolution X-ray spectroscopy, enabling most of the original X-IFU related scientific objectives of the Athena mission to be retained. (abridged)., Comment: 48 pages, 29 figures, Accepted for publication in Experimental Astronomy with minor editing
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- 2023
3. Transition-Edge Sensors for Cryogenic X-ray Imaging Spectrometers
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Luciano Gottardi and Stephen Smith
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- 2022
4. Progress in the Development of Frequency-Domain Multiplexing for the X-ray Integral Field Unit on Board the Athena Mission
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A. J. van den Linden, Mikko Kiviranta, Stephen J. Smith, J. van der Kuur, Kazuhiro Sakai, C. P. de Vries, Antoine R. Miniussi, Hiroki Akamatsu, Marcel P. Bruijn, K. Ravensberg, James A. Chervenak, Luciano Gottardi, Brian Jackson, and Nicholas A. Wakeham
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Transition-edge sensors ,Field (physics) ,FOS: Physical sciences ,LC circuit ,01 natural sciences ,Multiplexing ,010305 fluids & plasmas ,law.invention ,X-ray astronomy ,Optics ,law ,0103 physical sciences ,Athena ,General Materials Science ,Electronics ,010306 general physics ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Physics ,X-IFU ,business.industry ,Amplifier ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,X-ray calorimeters ,SQUID ,Astrophysics - Instrumentation and Methods for Astrophysics ,Alternating current ,business ,Energy (signal processing) - Abstract
Frequency domain multiplexing (FDM) is the baseline readout system for the X-ray Integral Field Unit (X-IFU) on board the Athena mission. Under the FDM scheme, TESs are coupled to a passive LC filter and biased with alternating current (AC bias) at MHz frequencies. Using high-quality factor LC filters and room temperature electronics developed at SRON and low-noise two-stage SQUID amplifiers provided by VTT, we have recently demonstrated good performance with the FDM readout of Mo/Au TES calorimeters with Au/Bi absorbers. We have achieved a performance requested for the demonstration model (DM) with the single pixel AC bias ($\Delta E=$1.8 eV) and 9 pixel multiplexing ($\Delta E=$2.6 eV) modes. We have also demonstrated 14-pixel multiplexing with an average energy resolution of 3.3 eV, which is limited by non-fundamental issues related to FDM readout in our lab setup., Comment: 7 pages, 5 figures. Published on Journal of Low Temperature Physics (2020)
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- 2020
5. Thermal Crosstalk of X-Ray Transition-Edge Sensor Micro-Calorimeters under Frequency Domain Multiplexing Readout
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Jan van der Kuur, Emanuele Taralli, Jan-Willem den Herder, Martin de Wit, K. Nagayoshi, D. Vaccaro, Hiroki Akamatsu, K. Ravensberg, Roland H. den Hartog, Ton Van der Linden, M. P. Bruijn, Jian-Rong Gao, Luciano Gottardi, Marcel L. Ridder, and Ruud W. M. Hoogeveen
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Physics - Instrumentation and Detectors ,Materials science ,detector energy resolution ,FOS: Physical sciences ,Signal ,Multiplexing ,x-ray astronomy ,space-borne satellites ,transition-edge sensors ,Electrical and Electronic Engineering ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Noise-equivalent power ,thermal crosstalk ,business.industry ,monte carlo ,Detector ,Instrumentation and Detectors (physics.ins-det) ,Condensed Matter Physics ,Chip ,Electronic, Optical and Magnetic Materials ,frequency domain multiplexing ,Crosstalk (biology) ,X-ray micro-calorimeters ,Optoelectronics ,Transition edge sensor ,Astrophysics - Instrumentation and Methods for Astrophysics ,business ,Degradation (telecommunications) - Abstract
We have measured and characterized the thermal crosstalk in two different arrays of transition-edge sensor (TES) X-ray micro-calorimeters with frequency-domain multiplexing (FDM) readout. The TES arrays are fabricated at SRON and are a 8$\times$8 and a 32$\times$32 "kilo-pixel" uniform array. The amount of crosstalk is evaluated as the ratio between the averaged crosstalk signal and the X-ray pulse amplitudes. The crosstalk ratios (CR) for our detectors are compliant with the requirements for future X-ray space missions, such as Athena X-IFU (CR$< 10^{-3}$ for first-neighbour pixels): we measured a nearest-neighbour thermal crosstalk ratio at a level of $10^{-4}$, with a highest crosstalk ratio of $4\times 10^{-4}$ for the kilo-pixel array (worst case, center of array) and $1\times 10^{-4}$ for the 8$\times$8 array, with a margin of improvement achievable by optimizing the Cu metallization and the width of the Si supporting structures (muntins) in the backside of the TES array chip. Based on the measured crosstalk ratios, we have estimated the impact on the spectral resolution by means of noise equivalent power (NEP) considerations and a Monte Carlo simulation, finding an average degradation in quadrature of less than 40~meV, compliant with the < 0.2~eV requirement for Athena X-IFU.
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- 2022
6. Demonstration of MHz frequency domain multiplexing readout of 37 transition edge sensors for high-resolution x-ray imaging spectrometers
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Mikko Kiviranta, B. J. van Leeuwen, Marcel L. Ridder, P. van der Hulst, A. C. T. Nieuwenhuizen, J. van der Kuur, D. Vaccaro, P. van Winden, S. Visser, K. Ravensberg, Brian Jackson, Ruud W. M. Hoogeveen, K. Nagayoshi, M. D'Andrea, J. W. den Herder, C. P. de Vries, A. J. van der Linden, R. den Hartog, M. de Wit, M. P. Bruijn, J. R. Gao, Hiroki Akamatsu, Emanuele Taralli, Luciano Gottardi, and Alec J. McCalden
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Superconductivity ,Physics ,Physics - Instrumentation and Detectors ,Physics and Astronomy (miscellaneous) ,Spectrometer ,Pixel ,business.industry ,FOS: Physical sciences ,Instrumentation and Detectors (physics.ins-det) ,Multiplexing ,law.invention ,SQUID ,Resonator ,law ,Optoelectronics ,Spectral resolution ,Transition edge sensor ,business ,Astrophysics - Instrumentation and Methods for Astrophysics ,Instrumentation and Methods for Astrophysics (astro-ph.IM) - Abstract
We report on the development and demonstration of a MHz frequency domain multiplexing (FDM) technology to read out arrays of cryogenic transition edge sensor (TES) X-ray microcalorimeters. In our FDM scheme, TESs are AC-biased at different resonant frequencies in the low MHz range through an array of high-$Q$ LC resonators. The current signals of all TESs are summed at superconducting quantum interference devices (SQUIDs). We have demonstrated multiplexing for a readout of 31 pixels using room temperature electronics, high-$Q$ LC filters and TES arrays developed at SRON, and SQUID arrays from VTT. We repeated this on a second setup with 37 pixels. The summed X-ray spectral resolutions $@$ 5.9 keV are $\Delta E_{\rm 31 pix ~MUX}=2.14\pm0.03$ eV and $\Delta E_{\rm 37 pix ~MUX}=2.23\pm0.03$ eV. The demonstrated results are comparable with other multiplexing approaches. There is potential to further improve the spectral resolution and to increase the number of multiplexed TESs, and to open up applications for TES X-ray microcalorimeters., Comment: 6 pages, 3 figures, accepted for publication on Applied physics letters
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- 2021
7. Time-Domain Modeling of TES Microcalorimeters Under AC Bias
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Jörn Wilms, Maximilian Lorenz, P. Peille, Thomas Dauser, R. den Hartog, Samuel Smith, Christian Kirsch, Brian Jackson, and Luciano Gottardi
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Physics ,Pixel ,Field (physics) ,Physics::Instrumentation and Detectors ,Differential equation ,Detector ,Astrophysics::Instrumentation and Methods for Astrophysics ,Condensed Matter Physics ,01 natural sciences ,Signal ,Atomic and Molecular Physics, and Optics ,010305 fluids & plasmas ,Computational physics ,Pulse (physics) ,0103 physical sciences ,General Materials Science ,Time domain ,010306 general physics - Abstract
We present developments in the simulation of transition-edge sensor (TES) microcalorimeters under AC bias for the purpose of detector studies. The presented model extends the TES differential equation system by describing the TES as a resistively shunted junction, using the Josephson equations instead of a parametrized resistance. To demonstrate the performance of this model, we compare simulated and measured IV curves of a pixel characterized for the Athena X-ray Integral Field Unit and showcase the signal generated by a simulated X-ray pulse.
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- 2019
8. Characterization of High Aspect-Ratio TiAu TES X-ray Microcalorimeter Array Under AC Bias
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Emanuele Taralli, Luciano Gottardi, K. Nagayoshi, M. P. Bruijn, Pourya Khosropanah, S. Visser, H. Akamatsu, J. R. Gao, M. Ridder, and J. van der Kuur
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Physics ,Fabrication ,business.industry ,Resolution (electron density) ,Detector ,Ranging ,Plasma ,Condensed Matter Physics ,7. Clean energy ,01 natural sciences ,Aspect ratio (image) ,Atomic and Molecular Physics, and Optics ,Space exploration ,010305 fluids & plasmas ,Optics ,0103 physical sciences ,General Materials Science ,010306 general physics ,business ,Energy (signal processing) - Abstract
We are developing X-ray microcalorimeters as a backup option for the baseline detectors in the X-IFU instrument on board the ATHENA space mission led by ESA and to be launched in the early 2030s.5$\times$5 mixed arrays with TiAu transition-edge sensor (TES), which have different high aspect ratios and thus high resistances, have been designed and fabricated to meet the energy resolution requirement of the X-IFU instrument. Such arrays can also be used to optimise the performance of the Frequency Domain Multiplexing (FDM) readout and lead to the final steps for the fabrication of a large detector array. In this work we present the experimental results from tens of the devices with an aspect ratio (length-to-width) ranging from 1-to-1 up to 6-to-1, measured in a single-pixel mode with a FDM readout system developed at SRON/VTT. We observed a nominal energy resolution of about 2.5 eV at 5.9 keV at bias frequencies ranging from 1 to 5 MHz. These detectors are proving to be the best TES microcalorimeters ever reported in Europe, being able to meet not only the requirements of the X-IFU instrument, but also those of other future challenging X-ray space missions, fundamental physics experiments, plasma characterization and material analysis.
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- 2019
9. Intrinsic Losses and Noise of High-Q Lithographic MHz LC Resonators for Frequency Division Multiplexing
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A. J. van der Linden, R. den Hartog, Luciano Gottardi, Mikko Kiviranta, K. Ravensberg, Hiroki Akamatsu, M. P. Bruijn, and J. van der Kuur
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FDM ,Thermal noise ,Transition-edge sensor ,Inductor ,01 natural sciences ,Noise (electronics) ,010305 fluids & plasmas ,law.invention ,Resonator ,law ,0103 physical sciences ,General Materials Science ,010306 general physics ,High-Q LC resonator ,Physics ,business.industry ,Amplifier ,Astrophysics::Instrumentation and Methods for Astrophysics ,OtaNano ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,SQUID ,Capacitor ,Electromagnetic coil ,Optoelectronics ,Transition edge sensor ,business - Abstract
We are developing the frequency division multiplexing (FDM) read-out for the superconducting transition-edge sensors arrays of the X-IFU instrument on board of Athena and of the SAFARI instrument on board of SPICA. An essential component of the FDM is the array of narrow band superconducting resonators, each consisting of lithographically made inductors and capacitors. In the standard FDM configuration, the LC resonators are connected in series with the input coil of a low noise two-stage SQUID amplifier. In this work, we have modified the electrical scheme to weakly couple the SQUID amplifier from the LC filters in order to measure their intrinsic properties. We report on the intrinsic losses and on the noise of high-Q superconducting LC resonators, with resonant frequencies ranging between 1 and 5 MHz, measured at temperatures from 70 to 500 mK. The LC resonators show very low losses with values smaller than $$0.5\,\mathrm {m}\Omega $$ at equilibrium temperatures below 100 mK. We demonstrate that the LC resonators noise is thermal between 500 and 70 mK.
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- 2019
10. Voltage Fluctuations in ac Biased Superconducting Transition-Edge Sensors
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A. G. Kozorezov, K. Nagayashi, Luciano Gottardi, Emanuele Taralli, and M. de Wit
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Superconductivity ,Physics ,Resistive touchscreen ,Condensed matter physics ,Condensed Matter - Superconductivity ,Detector ,FOS: Physical sciences ,General Physics and Astronomy ,Johnson–Nyquist noise ,02 engineering and technology ,021001 nanoscience & nanotechnology ,01 natural sciences ,Superconductivity (cond-mat.supr-con) ,Harmonics ,0103 physical sciences ,Quasiparticle ,Astrophysics - Instrumentation and Methods for Astrophysics ,010306 general physics ,0210 nano-technology ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Noise (radio) ,Voltage - Abstract
We present a detailed analysis of the fundamental noise sources in superconducting transition-edge sensors (TESs), ac voltage biased at MHz frequencies and treated as superconducting weak links. We have studied the noise in the resistive transition as a function of bath temperature of several detectors with different normal resistances and geometries. We show that the excess noise, typically observed in the TES electrical bandwidth, can be explained by the equilibrium Johnson noise of the quasiparticles generated within the weak link. The fluctuations at the Josephson frequency and higher harmonics contribute significantly to the measured voltage noise at the detector bandwidth through the nonlinear response of the weak link with a sinusoidal current-phase relation., 9 pages, 7 figures
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- 2021
11. A Review of X-ray Microcalorimeters Based on Superconducting Transition Edge Sensors for Astrophysics and Particle Physics
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Kenichiro Nagayashi and Luciano Gottardi
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Particle physics ,Technology ,Fabrication ,Physics::Instrumentation and Detectors ,neutrino mass experiments ,QH301-705.5 ,QC1-999 ,FOS: Physical sciences ,02 engineering and technology ,Astrophysics ,low temperature detectors ,01 natural sciences ,Superconductivity (cond-mat.supr-con) ,superconducting detectors ,detectors for particle physics ,0103 physical sciences ,General Materials Science ,Biology (General) ,010306 general physics ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Instrumentation ,Transition edge ,QD1-999 ,Fluid Flow and Transfer Processes ,Physics ,Superconductivity ,Pixel ,Condensed Matter - Superconductivity ,Process Chemistry and Technology ,Detector ,General Engineering ,X-ray microcalorimeters ,021001 nanoscience & nanotechnology ,Engineering (General). Civil engineering (General) ,Superconducting detectors ,Computer Science Applications ,Chemistry ,solar axions ,TA1-2040 ,Astrophysics - Instrumentation and Methods for Astrophysics ,0210 nano-technology - Abstract
The state-of-the-art technology of X-ray microcalorimeters based on superconducting transition edge sensors (TESs), for applications in astrophysics and particle physics, is reviewed. We will show the advance in understanding the detector physics and describe the recent breakthroughs in the TES design that are opening the way towards the fabrication and the read-out of very large arrays of pixels with unprecedented energy resolution. The most challenging low temperature instruments for space- and ground-base experiments will be described., 48 pages, 14 figures, published in Appl. Sci. 2021, 11, 3793
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- 2021
12. Impact of the Absorber-Coupling Design for Transition-Edge-Sensor X-Ray Calorimeters
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Marcel L. Ridder, D. Vaccaro, Emanuele Taralli, K. Ravensberg, Hiroki Akamatsu, Ruud W. M. Hoogeveen, M. de Wit, K. Nagayoshi, J. van der Kuur, J. W. den Herder, Luciano Gottardi, M. P. Bruijn, and J. R. Gao
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Superconductivity ,Coupling ,Physics - Instrumentation and Detectors ,Materials science ,business.industry ,Bilayer ,Astrophysics::Instrumentation and Methods for Astrophysics ,General Physics and Astronomy ,FOS: Physical sciences ,Instrumentation and Detectors (physics.ins-det) ,Noise (electronics) ,Power (physics) ,Optics ,Thermal ,Transition edge sensor ,Astrophysics - Instrumentation and Methods for Astrophysics ,business ,Electrical impedance ,Instrumentation and Methods for Astrophysics (astro-ph.IM) - Abstract
Transition Edge Sensors (TESs) are the selected technology for future spaceborne X-ray observatories, such as Athena, Lynx, and HUBS. These missions demand thousands of pixels to be operated simultaneously with high energy-resolving power. To reach these demanding requirements, every aspect of the TES design has to be optimized. Here we present the experimental results of tests on different devices where the coupling between the x-ray absorber and the TES sensor is varied. In particular, we look at the effects of the diameter of the coupling stems and the distance between the stems and the TES bilayer. Based on measurements of the AC complex impedance and noise, we observe a reduction in the excess noise as the spacing between the absorber stem and the bilayer is decreased. We identify the origin of this excess noise to be internal thermal fluctuation noise between the absorber stem and the bilayer. Additionally, we see an impact of the coupling on the superconducting transition in the appearance of kinks. Our observations show that these unwanted structures in the transition shape can be avoided with careful design of the coupling geometry. Also the stem diameter appears to have a significant impact on the smoothness of the TES transition. This observation is still poorly understood, but is of great importance for both AC and DC biased TESs., Comment: 9 pages, 8 figures
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- 2021
13. TiAu TES 32$\times$32 pixel array: uniformity, thermal crosstalk and performance at different X-ray energies
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Luciano Gottardi, K. Nagayoshi, Marcel L. Ridder, M. D'Andrea, Martin de Wit, Ruud W. M. Hoogeveen, Hiroki Akamatsu, D. Vaccaro, K. Ravensberg, S. Visser, M. P. Bruijn, Emanuele Taralli, and Jian-Rong Gao
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Physics - Instrumentation and Detectors ,Photon ,Physics::Instrumentation and Detectors ,Astrophysics::High Energy Astrophysical Phenomena ,FOS: Physical sciences ,Large format ,7. Clean energy ,01 natural sciences ,Optics ,0103 physical sciences ,Electrical and Electronic Engineering ,010306 general physics ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Physics ,business.industry ,Detector ,Astrophysics::Instrumentation and Methods for Astrophysics ,Order (ring theory) ,Instrumentation and Detectors (physics.ins-det) ,Condensed Matter Physics ,Electronic, Optical and Magnetic Materials ,Full width at half maximum ,Amplitude ,Transition edge sensor ,Astrophysics - Instrumentation and Methods for Astrophysics ,business ,Energy (signal processing) - Abstract
Large format arrays of transition edge sensor (TES) are crucial for the next generation of X-ray space observatories. Such arrays are required to achieve an energy resolution of $\mathrm{\Delta }E 3 eV full-width-half-maximum (FWHM) in the soft X-ray energy range. We are currently developing X-ray microcalorimeter arrays as a backup option for the X-IFU instrument on board of ATHENA space telescope, led by ESA and foreseen to be launched in 2031. In this contribution, we report on the development and the characterization of a uniform 32 × 32 pixel array with (length × width) 140 × 30 $\mu$ m $^2$ TiAu TESs, which have a 2.3 $\mu$ m thick Au absorber for X-ray photons. The pixels have a typical normal resistance $R_{\mathrm{n}}$ = 121 m $\Omega$ and a critical temperature $T_{\mathrm{c}}\sim$ 90 mK. We performed extensive measurements on 60 pixels out of the array in order to show the uniformity of the array. We obtained an energy resolutions between 2.4 and 2.6 eV (FWHM) at 5.9 keV, measured in a single-pixel mode at AC bias frequencies ranging from 1 to 5 MHz, with a frequency domain multiplexing (FDM) readout system, which is developed at SRON/VTT. We also present the detector energy resolution at X-ray with different photon energies generated by a modulated external X-ray source from 1.45 keV up to 8.9 keV. Multiplexing readout across several pixels has also been performed to evaluate the impact of the thermal crosstalk to the instrument's energy resolution budget requirement. This value results in a derived requirement, for the first neighbour, that is less than 1 $\;\times\; 10^{-3}$ when considering the ratio between the amplitude of the crosstalk signal to an X-ray pulse (for example at 5.9 keV).
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- 2021
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14. Single Pixel Performance of a 32 x 32 Ti/Au TES Array With Broadband X-Ray Spectra
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Hiroki Akamatsu, Marcel L. Ridder, M. D'Andrea, Kenichiro Nagayoshi, K. Ravensberg, Luciano Gottardi, Jian-Rong Gao, Ruud W. M. Hoogeveen, Cor P. de Vries, D. Vaccaro, Emanuele Taralli, Martin de Wit, and Marcel P. Bruijn
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Physics - Instrumentation and Detectors ,Photon ,Physics::Instrumentation and Detectors ,Astrophysics::High Energy Astrophysical Phenomena ,energy resolution ,FOS: Physical sciences ,01 natural sciences ,0103 physical sciences ,Calibration ,Energy calibration ,Electrical and Electronic Engineering ,010306 general physics ,Electronic band structure ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Line (formation) ,Physics ,X-IFU ,x-ray detectors ,Detector ,Linearity ,Instrumentation and Detectors (physics.ins-det) ,Condensed Matter Physics ,Electronic, Optical and Magnetic Materials ,Computational physics ,Full width at half maximum ,MXS ,Astrophysics - Instrumentation and Methods for Astrophysics ,TES ,Energy (signal processing) - Abstract
We are developing a kilo-pixels Ti/Au TES array as a backup option for Athena X-IFU. Here we report on single-pixel performance of a 32$\times$32 array operated in a Frequency Division Multiplexing (FDM) readout system, with bias frequencies in the range 1-5 MHz. We have tested the pixels response at several photon energies, by means of a $^{55}$Fe radioactive source (emitting Mn-K$\alpha$ at 5.9 keV) and a Modulated X-ray Source (MXS, providing Cr-K$\alpha$ at 5.4 keV and Cu-K$\alpha$ at 8.0 keV). First, we report the procedure used to perform the detector energy scale calibration, usually achieving a calibration accuracy better than $\sim$ 0.5 eV in the 5.4 - 8.9 keV energy range. Then, we present the measured energy resolution at the different energies (best single pixel performance: $\Delta$E$_{FWHM}$ = 2.40 $\pm$ 0.09 eV @ 5.4 keV; 2.53 $\pm$ 0.10 eV @ 5.9 keV; 2.78 $\pm$ 0.16 eV @ 8.0 keV), investigating also the performance dependency from the pixel bias frequency and the count rate. Thanks to long background measurements ($\sim$ 1 day), we finally detected also the Al-K$\alpha$ line at 1.5 keV, generated by fluorescence inside the experimental setup. We analyzed this line to obtain a first assessment of the single-pixel performance also at low energy ($\Delta$E$_{FWHM}$ = 1.91 eV $\pm$ 0.21 eV @ 1.5 keV), and to evaluate the linearity of the detector response in a large energy band (1.5 - 8.9 keV)., Comment: Accepted for publication in IEEE Transactions on Applied Superconductivity for ASC2020 special issue
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- 2021
15. A test platform for the detection and readout chain for the Athena X-IFU
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Kazuhiro Sakai, Mikko Kiviranta, François Pajot, G. Roudil, Edoardo Cucchetti, William B. Doriese, Gabriele Betancourt-Martinez, Michel Dupieux, Sophie Beaumont, Stephen J. Smith, L. Ravera, Carl D. Reintsema, Antoine R. Miniussi, B. D. Jackson, Joseph D. Adams, Hiroki Akamatsu, Florent Castellani, Marcel P. Bruijn, K. Ravensberg, Nicholas A. Wakeham, Luciano Gottardi, P. Peille, Jan van der Kuur, M. C. Witthoeft, Doreen Wernicke, Hervé Geoffray, Bernard Bertrand, Simon R. Bandler, Henk van Weers, Institut de recherche en astrophysique et planétologie (IRAP), Institut national des sciences de l'Univers (INSU - CNRS)-Université Toulouse III - Paul Sabatier (UT3), Université Fédérale Toulouse Midi-Pyrénées-Université Fédérale Toulouse Midi-Pyrénées-Observatoire Midi-Pyrénées (OMP), Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Centre National de la Recherche Scientifique (CNRS), and Centre National d'Études Spatiales [Toulouse] (CNES)
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Cryostat ,Test bench ,Physics - Instrumentation and Detectors ,Spectrometer ,Computer science ,business.industry ,Readout electronics ,FOS: Physical sciences ,02 engineering and technology ,Instrumentation and Detectors (physics.ins-det) ,021001 nanoscience & nanotechnology ,01 natural sciences ,010309 optics ,Test platform ,0103 physical sciences ,Calibration ,Electronics ,[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det] ,Astrophysics - Instrumentation and Methods for Astrophysics ,0210 nano-technology ,business ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Computer hardware - Abstract
We present a test platform for the Athena X-IFU detection chain, which will serve as the first demonstration of the representative end-to-end detection and readout chain for the X-IFU, using prototypes of the future flight electronics and currently available subsystems. This test bench, housed in a commercial two-stage ADR cryostat, includes a focal plane array placed at the 50 mK cold stage of the ADR with a kilopixel array of transition-edge sensor microcalorimeter spectrometers and associated cold readout electronics. Prototype room temperature electronics for the X-IFU provide the readout, and will evolve over time to become more representative of the X-IFU mission baseline. The test bench yields critical feedback on subsystem designs and interfaces, in particular the warm readout electronics, and will provide an in-house detection system for continued testing and development of the warm readout electronics and for the validation of X-ray calibration sources. In this paper, we describe the test bench subsystems and design, characterization of the cryostat, and current status of the project., Comment: 11 pages, 4 figures, to appear in Proc. SPIE Astronomical Telescopes and Instrumentation, 2020
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- 2020
16. Frequency domain multiplexing technology of transition-edge sensors for x-ray astronomy
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Hiroki Akamatsu, Davide Vaccaro, Luciano Gottardi, Jan van der Kuur, Cor P. de Vries, Simon R. Bandler, Marcel P. Bruijn, James A. Chervenak, Matteo D'Andrea, Jian-Rong Gao, Jan-Willem A. den Herder, Ruud W. M. Hoogeveen, Mikko Kiviranta, Anton J. van der Linden, Brian D. Jackson, Antoine R. Miniussi, Kenichiro Nagayoshi, Kevin Ravensberg, Marcel L. Ridder, Kazuhiro Sakai, Stephen J. Smith, Emanuele Taralli, Sven Visser, Nicholas A. Wakeham, and Martin de Wit
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Physics ,X-ray astronomy ,business.industry ,Frequency domain multiplexing ,Electrical engineering ,Multiplexing ,law.invention ,On board ,SQUID ,law ,Observatory ,Satellite ,business ,Transition edge - Abstract
We are developing Frequency Domain Multiplexing (FDM) read-out of Transition-Edge Sensors (TESs) for the X-ray Integral Field Unit (X-IFU) on board of the future European X-Ray observatory Athena. The X-IFU Focal-Plane Assembly consists of a $sim$ 3000-pixel array, read out by SQUID-based FDM. The multiplexing readout scheme is a critical technology for the X-IFU instrument because of the cooling and electronic power limits for the satellite. In this contribution, we report on the development of FDM readout technology and on the performance of TESs array under an AC bias at MHz frequencies.
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- 2020
17. Development of microwave multiplexer for the Super DIOS mission: 38 transition-edge sensor x-ray microcalorimeter readout with microwave multiplexing
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Luciano Gottardi, M. P. Bruijn, Shinya Yamada, Jian-Rong Gao, Hiroki Akamatsu, Satoshi Kohjiro, Noriko Yamasaki, Akira Sato, Jan-Willem den Herder, Fuminori Hirayama, Kenichiro Nagayoshi, Ryota Hayakawa, Emanuele Taralli, Kazuhisa Mitsuda, Marcel L. Ridder, Yuki Nakashima, Shuichi Nagasawa, and Hirotake Yamamori
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Physics ,Pixel ,Physics::Instrumentation and Detectors ,business.industry ,Detector ,Astrophysics::Instrumentation and Methods for Astrophysics ,Imaging spectrometer ,Multiplexer ,Multiplexing ,Optics ,Angular resolution ,Transition edge sensor ,business ,Microwave - Abstract
We are developing an x-ray imaging spectrometer for Super DIOS satellite mission, a future x-ray observatory, planned by JAXA, to be launched in 2030’s. Super DIOS will reveal the nature of the missing baryon in the warm-hot intergalactic medium because of its fine energy and angular resolution, large effective area and large field of view. A main detector on-board Super DIOS consists of a transition-edge sensor (TES) microcalorimeter array of over 30,000 pixels working at a temperature below 100 mK and it poses a considerable technical difficulty to the readout. A microwave superconducting quantum interference device (SQUID) multiplexing is promising technique and expected to achieve a large scale readout of more than 30,000 pixels. We describe our development of a 40-channel microwave SQUID multiplexer with low-noise characteristics∗ and a demonstration of simultaneously reading out 40-pixel TESs. Finally, we discuss a future prospect and a feasibility of reading out an array of more than 30,000 pixels.
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- 2020
18. HUBS: a dedicated hot circumgalactic medium explorer
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Wei Cui, Joel Bregman, Marcel Bruijin, Liubiao Chen, Yang Chen, Chen Cui, Taotao Fang, Bo Gao, He Gao, Jian-Rong Gao, Luciano Gottardi, Kaixuan Gu, Fulai Guo, Jia Guo, Chunling He, Pengfei He, Jan-Willem A. den Herder, Qiushi Huang, Fajun Li, Jiangtao Li, Jinjin Li, Lingyun Li, Tipei Li, Wenbing Li, Jingtao Liang, Yajie Liang, Guiyun Liang, Yanjie Liu, Zhi Liu, Ziyao Liu, Felix Jaeckel, Li Ji, Wei Ji, Hai Jin, Xi Kang, Yuexue Ma, Dan McCammon, Houjun Mo, Kenichiro Nagayoshi, Kari Nelms, Ruizhe Qi, Jia Quan, Marcel Ridder, Zhengxiang Shen, Aurora Simionescu, Emanuele Taralli, Daniel Wang, Guole Wang, Junjie Wang, Kun Wang, Le Wang, Sifan Wang, Shijian Wang, Tinggui Wang, Wei Wang, Xiaoqiang Wang, Yongliang Wang, Yeru Wang, Zhen Wang, Zhanshan Wang, Ningyuan Wen, Martin de Wit, Shufan Wu, Da Xu, Dandan Xu, Haiguang Xu, Xiaojie Xu, Renxin Xu, Yongquan Xue, Shengzhen Yi, Jun Yu, Luwei Yang, Feng Yuan, Shuo Zhang, Wei Zhang, Zhong Zhang, Qing Zhong, Yu Zhou, and Wenxiu Zhu
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Physics ,Void (astronomy) ,Astrophysics::High Energy Astrophysical Phenomena ,media_common.quotation_subject ,Dark matter ,FOS: Physical sciences ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,01 natural sciences ,Universe ,Galaxy ,Baryon ,Stars ,0103 physical sciences ,Galaxy formation and evolution ,Astrophysics - Instrumentation and Methods for Astrophysics ,010306 general physics ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,010303 astronomy & astrophysics ,Astrophysics::Galaxy Astrophysics ,Galaxy cluster ,media_common - Abstract
The Hot Universe Baryon Surveyor (HUBS) mission is proposed to study "missing" baryons in the universe. Unlike dark matter, baryonic matter is made of elements in the periodic table, and can be directly observed through the electromagnetic signals that it produces. Stars contain only a tiny fraction of the baryonic matter known to be present in the universe. Additional baryons are found to be in diffuse (gaseous) form, in or between galaxies, but a significant fraction has not yet been seen. The latter (missing baryons) are thought to be hiding in low-density warm-hot ionized medium (WHIM), based on results from theoretical studies and recent observations, and be distributed in the vicinity of galaxies (i.e., circum-galactic medium) and between galaxies (i.e., intergalactic medium). Such gas would radiate mainly in the soft X-ray band and the emission would be very weak, due to its very low density. HUBS is optimized to detect the X-ray emission from the hot baryons in the circum-galactic medium, and thus fill a void in observational astronomy. The goal is not only to detect the missing baryons, but to characterize their physical and chemical properties, as well as to measure their spatial distribution. The results would establish the boundary conditions for understanding galaxy evolution. Though highly challenging, detecting missing baryons in the intergalactic medium could be attempted, perhaps in the outskirts of galaxy clusters, and could shed significant light on the large-scale structures of the universe. The current design of HUBS will be presented, along with the status of technology development., Comment: 12 pages, 7 figures, Space Telescopes and Instrumentation 2020: Ultraviolet to Gamma Ray, eds. J.A. den Herder, S. Nikzad, & K. Nakazawa, Proc. of SPIE Vol. 11444, 114442S
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- 2020
19. Developing x-ray microcalorimeters based on TiAu TES for HUBS
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Marcel L. Ridder, Hiroki Akamatsu, M. P. Bruijn, K. Nagayoshi, J. R. Gao, G. Wang, Luciano Gottardi, J. W. den Herder, Emanuele Taralli, and Wei Cui
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Physics ,Photon ,Spectrometer ,Pixel ,Physics::Instrumentation and Detectors ,business.industry ,Resolution (electron density) ,Astrophysics::Instrumentation and Methods for Astrophysics ,Field of view ,Optics ,Thermal ,Angular resolution ,Transition edge sensor ,business - Abstract
Hot Universe Baryon Surveyor (HUBS), a Chinese space mission, is proposed to find a large fraction of the so-called missing baryons, which would help us to understand more about the structure formation and evolution of the universe. Both theoretical and experimental results show that developing a highly efficient soft X-ray spectrometer over a large field of view and with a high energy resolution is the key to detect the “missing baryons”. X-ray microcalorimeters based on a transition-edge sensor (TES) array is required for HUBS, which aims to have 1 deg2 field of view (FoV) with 1’ angular resolution and 2 eV energy resolution optimized around 0.6 keV. Taking the high throughput X-ray optical focusing system on HUBS into account, the TES array is designed to have 60 x 60 pixels with an area of 1 mm2 for each pixel. The microcalorimeter consists of a TES, a weak thermal link to a heat bath, and a semi-metal or normal metal absorber to increase the X-ray absorption efficiency. When an X-ray photon with a given energy is absorbed, the temperature of the absorber increase, that can be monitored by measuring the resistance change of the TES. A bilayer of a superconductor and a normal metal is used to fabricate a TES with a critical temperature (Tc) of ~100 mK. The latter is set for the required energy resolution. For HUBS, both MoCu and TiAu TES technologies are considered in its development phase. Here we will focus on TiAu TES calorimeters designed and partially fabricated at SRON for HUBS. Recent demonstration of a resolution of 2.5 eV at 5.9 keV in an AC readout at SRON for X-IFU on board of Athena illustrates the promising of this technology. However, the challenging for the HUBS array is the large pixel size. We will report the design and fabrication of prototype HUBS calorimeters.
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- 2020
20. Study of TES Detector Transition Curve to Optimize the Pixel Design for Frequency-Division Multiplexing Readout
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M. P. Bruijn, Marcel L. Ridder, K. Nagayoshi, A. C. T. Nieuwenhuizen, Emanuele Taralli, K. Ravensberg, Luciano Gottardi, Hiroki Akamatsu, J. van der Kuur, J. R. Gao, S. Visser, J. W. den Herder, and Pourya Khosropanah
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Physics ,Superconductivity ,Transition-edge sensors ,Pixel ,business.industry ,Physics::Instrumentation and Detectors ,Detector ,Resolution (electron density) ,Astrophysics::Instrumentation and Methods for Astrophysics ,Frequency-domain multiplexing ,Condensed Matter Physics ,01 natural sciences ,Weak link ,Atomic and Molecular Physics, and Optics ,010305 fluids & plasmas ,Frequency-division multiplexing ,0103 physical sciences ,Limit (music) ,Optoelectronics ,General Materials Science ,Spectral resolution ,010306 general physics ,business ,Energy (signal processing) - Abstract
Superconducting transition-edge sensors (TESs) are highly sensitive detectors. Based on the outstanding performance on spectral resolution, the X-ray integral field unit (X-IFU) instrument on-board athena will be equipped with a large array of TES-based microcalorimeters. For optimal performance in terms of the energy resolution, it is essential to limit undesirable nonlinearity effects in the TES detector. Weak-link behavior induced on the TES by superconducting leads is such a nonlinearity effect. We designed and fabricated smart test structures to study the effect of the superconducting leads on the intrinsic transition curve of our TiAu-based TES bilayer. We measured and analyzed the resistance versus temperature transition curves of the test structures. We found relations of long-distance proximity effects with TES length and different lead materials. Based on these results, we can redesign and further optimize our TES-based X-ray detectors.
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- 2020
21. Characterization of a Ti/Au TES with Au/Bi absorber under AC and DC bias
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Carlos Pobes, Kenichiro Nagayoshi, Pourya Khosropanah, Luciano Gottardi, Agustín Camón, Jian-Rong Gao, Marcel P. Bruijn, Lourdes Fàbrega, Emanuele Taralli, Marcel L. Ridder, European Space Agency, European Commission, Ministerio de Economía y Competitividad (España), Agencia Estatal de Investigación (España), and Ministerio de Ciencia, Innovación y Universidades (España)
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Physics - Instrumentation and Detectors ,Materials science ,Transition-edge sensor ,FOS: Physical sciences ,Complex impedance ,7. Clean energy ,01 natural sciences ,Noise (electronics) ,Multiplexing ,010305 fluids & plasmas ,0103 physical sciences ,General Materials Science ,010306 general physics ,AC bias and DC bias ,Pixel ,business.industry ,X-ray ,Biasing ,Instrumentation and Detectors (physics.ins-det) ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,Characterization (materials science) ,Wavelength ,Optoelectronics ,business ,DC bias - Abstract
Transition-edge sensors (TESs) are used as very sensitive thermometers in microcalorimeters aimed at detection of different wavelengths. In particular, for soft X-ray astrophysics, science goals require very high-resolution microcalorimeters which can be achieved with TESs coupled to suitable absorbers. For many applications, there is also need for a high number of pixels which typically requires multiplexing in the readout stage. Frequency-domain multiplexing (FDM) is a common scheme and is the baseline proposed for the ATHENA mission. FDM requires biasing the TES in AC at MHz frequencies. Recently, there has been reported degradation in performances under AC with respect to DC bias. In order to assess the performances of TESs to be used with FDM, it is thus of great interest to compare the performances of the same device both under AC bias and DC bias. This requires two different measurement set-ups with different processes for making the characterization. We report in this work the preliminary results of a single-pixel characterization performed on a TiAu TES under AC and afterwards under DC bias in different facilities. Extraction of dynamical parameters and noise performances are compared in both cases as a first stage for further AC/DC comparison of these devices., This work is partly funded by European Space Agency (ESA) and coordinated with other European efforts under ESA CTP contract ITT AO/1-7947/14/NL/BW. It has also received funding from the European Union’s Horizon 2020 Programme under the AHEAD (Activities for the High-Energy Astrophysics Domain) project with grant agreement number 654215. CSIC work is financed by the Spanish Ministerio de Ciencia, Innovación y Universidades-MICINN (projects ESP2016-76683-C3-2-R and RTI2018-096686-B-C22). Personnel from ICMAB acknowledge financial support from MINECO, through the “Severo Ochoa” Programme for Centres of Excellence in R&D (SEV-2015-0496).
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- 2020
22. Study of Dissipative Losses in AC-Biased Mo/Au Bilayer Transition-Edge Sensors
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Nicholas A. Wakeham, F. M. Finkbeiner, A. J. van der Linden, Simon R. Bandler, R. L. Kelley, H. van Weers, Edward J. Wassell, Brian Jackson, Mikko Kiviranta, Kazuhiro Sakai, B. J. van Leeuwen, F. S. Porter, J. S. Sadleir, Wonsik Yoon, Hiroki Akamatsu, A. R. Miniussi, J. van der Kuur, Joseph S. Adams, Jay Chervenak, Stephen J. Smith, M. P. Bruijn, Caroline A. Kilbourne, Aaron M. Datesman, Megan E. Eckart, and Luciano Gottardi
- Subjects
Transition-edge sensors ,Materials science ,Field (physics) ,02 engineering and technology ,01 natural sciences ,law.invention ,law ,0103 physical sciences ,Eddy current ,Noise control ,Microcalorimeters ,General Materials Science ,010306 general physics ,Absorption (electromagnetic radiation) ,Eddy current heating ,Coupling ,OtaNano ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,Finite element method ,Computational physics ,Frequency-division multiplexing ,Dissipative system ,0210 nano-technology ,DC bias - Abstract
We are developing kilo-pixel arrays of transition-edge sensors (TESs) for the X-ray Integral Field Unit on ESA’s Athena observatory. Previous measurements of AC-biased Mo/Au TESs have highlighted a frequency-dependent loss mechanism that results in broader transitions and worse spectral performance compared to the same devices measured under DC bias. In order to better understand the nature of this loss, we are now studying TES pixels in different geometric configurations. We present measurements on devices of different sizes and with different metal features used for noise mitigation and X-ray absorption. Our results show how the loss mechanism is strongly dependent upon the amount of metal in close proximity to the sensor and can be attributed to induced eddy current coupling to these features. We present a finite element model that successfully reproduces the magnitude and geometry dependence of the losses. Using this model, we present mitigation strategies that should reduce the losses to an acceptable level.
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- 2018
23. Josephson Effects in Frequency-Domain Multiplexed TES Microcalorimeters and Bolometers
- Author
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Marcel P. Bruijn, Stephen J. Smith, M. Ridder, P. Khosropanah, A. R. Miniussi, J. van der Kuur, J. R. Gao, Jay Chervenak, Luciano Gottardi, Brian Jackson, N. Wakeham, R. den Hartog, H. Akamatsu, A. G. Kozorezov, Kazuhiro Sakai, K. Nagayoshi, John E. Sadleir, and Simon R. Bandler
- Subjects
Josephson effect ,Transition-edge sensors ,Frequency-domain multiplexing ,02 engineering and technology ,01 natural sciences ,Multiplexing ,law.invention ,law ,0103 physical sciences ,General Materials Science ,010306 general physics ,Electrical impedance ,Physics ,Superconductivity ,Resistive touchscreen ,business.industry ,Detector ,Bolometer ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,Frequency domain ,Optoelectronics ,0210 nano-technology ,business - Abstract
Frequency-division multiplexing is the baseline read-out system for large arrays of superconducting transition-edge sensors (TES’s) under development for the X-ray and infrared instruments like X-IFU (Athena) and SAFARI, respectively. In this multiplexing scheme, the sensors are ac-biased at different frequencies from 1 to 5 MHz and operate as amplitude modulators. Weak superconductivity is responsible for the complex TES resistive transition, experimentally explored in great detail so far, both with dc- and ac-biased read-out schemes. In this paper, we will review the current status of our understanding of the physics of the TES’s and their interaction with the ac bias circuit. In particular, we will compare the behaviour of the TES nonlinear impedance, across the superconducting transition, for several detector families, namely: high-normal-resistance TiAu TES bolometers, low-normal-resistance MoAu TES microcalorimeters and high-normal-resistance TiAu TES microcalorimeters.
- Published
- 2018
24. LC Filters for FDM Readout of the X-IFU TES Calorimeter Instrument on Athena
- Author
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M. P. Bruijn, Luciano Gottardi, Lorenza Ferrari, Hiroki Akamatsu, Brian Jackson, Roland H. den Hartog, Anton J. van der Linden, and Jan van der Kuur
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Materials science ,Fabrication ,Equivalent series resistance ,business.industry ,02 engineering and technology ,Experimental validation ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,01 natural sciences ,Atomic and Molecular Physics, and Optics ,Finite element method ,Calorimeter ,law.invention ,Capacitor ,Quality (physics) ,law ,0103 physical sciences ,Optoelectronics ,General Materials Science ,010306 general physics ,0210 nano-technology ,business ,Lithography - Abstract
The current status of lithographic superconducting LC filters for use in the Athena-X-IFU instrument is described. We present the fabrication process and characterization results at room temperature, 4 K and 50 mK. We also present an optimization study of the quality topics, where finite element modeling is used together with experimental validation structures. For the a-Si:H-based capacitors and Nb-based coils, presently the component fabrication yield is about 99% and the effective series resistance at 50 mK is lower than 1.5 mΩ.
- Published
- 2018
25. A six-degree-of-freedom micro-vibration acoustic isolator for low-temperature radiation detectors based on superconducting transition-edge sensors
- Author
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Johannes Dercksen, Pourya Khosropanah, Marcel L. Ridder, H. van Weers, K. Ravensberg, M. P. Bruijn, Luciano Gottardi, Hiroki Akamatsu, Brian Jackson, J. van der Kuur, and J. R. Gao
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010302 applied physics ,Materials science ,Physics::Instrumentation and Detectors ,business.industry ,Isolator ,Astrophysics::Instrumentation and Methods for Astrophysics ,Cryogenics ,Cryocooler ,01 natural sciences ,Particle detector ,010305 fluids & plasmas ,Pulse (physics) ,Vibration ,Optics ,0103 physical sciences ,Pulse tube refrigerator ,business ,Adiabatic process ,Instrumentation - Abstract
Dilution and adiabatic demagnetization refrigerators based on pulse tube cryocoolers are nowadays used in many low temperature physics experiments, such as atomic force and scanning tunneling microscopy, quantum computing, radiation detectors, and many others. A pulse tube refrigerator greatly simplifies the laboratory activities being a cryogen-free system. The major disadvantage of a pulse tube cooler is the high level of mechanical vibrations at the warm and cold interfaces that could substantially affect the performance of very sensitive cryogenic instruments. In this paper, we describe the performance of a very simple mechanical attenuation system used to eliminate the pulse-tube-induced low frequency noise of the superconducting transition-edge sensors under development for the instruments of the next generation of infra-red and X-ray space observatories.
- Published
- 2019
26. Complex impedance of TESs under AC bias using FDM readout system
- Author
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Marcel L. Ridder, Pourya Khosropanah, Kenichiro Nagayoshi, J. R. Gao, Luciano Gottardi, Marcel P. Bruijn, and Emanuele Taralli
- Subjects
010302 applied physics ,Physics ,Physics - Instrumentation and Detectors ,Pixel ,business.industry ,Physics::Instrumentation and Detectors ,Detector ,General Physics and Astronomy ,FOS: Physical sciences ,02 engineering and technology ,Instrumentation and Detectors (physics.ins-det) ,021001 nanoscience & nanotechnology ,01 natural sciences ,Noise (electronics) ,lcsh:QC1-999 ,Calorimeter ,Optics ,0103 physical sciences ,Sensitivity (control systems) ,Transition edge sensor ,0210 nano-technology ,business ,Electrical impedance ,lcsh:Physics ,DC bias - Abstract
The next generation of Far-infrared and X-ray space observatories will require detector arrays with thousands of transition edge sensor (TES) pixel. It is extremely important to have a tool that is able to characterize all the pixels and that can give a clear picture of the performance of the devices. In particular, we refer to those aspects that can affect the global energy resolution of the array: logarithmic resistance sensitivity with respect to temperature and current (α and β parameters, respectively), uniformity of the TESs and the correct understanding of the detector thermal model. Complex impedance measurement of a TES is the only technique that can give all this information at once, but it has been established only for a single pixel under DC bias. We have developed a complex impedance measurement method for TESs that are AC biased since we are using a MHz frequency domain multiplexing (FDM) system to readout an array. The FDM readout demands for some modifications to the complex-impedance technique and extra considerations, e.g. how to modulate a small fraction of the bias carrier frequencies in order to get a proper excitation current through the TESs and how to perform an accurate demodulation and recombination of the output signals. Also, it requires careful calibration to remove the presence of parasitic impedances in the entire readout system. We perform a complete set of AC impedance measurements for different X-ray TES microcalorimeters based on superconducting TiAu bilayers with or without normal metal Au bar structures. We discuss the statistical analysis of the residual between impedance data and fitting model to determine the proper calorimeter thermal model for our detectors. Extracted parameters are used to improve our understanding of the differences and capabilities among the detectors and additionally the quality of the array. Moreover, we use the results to compare the calculated noise spectra with the measured data.
- Published
- 2019
27. Development of a Ti/Au TES Microcalorimeter Array as a Backup Sensor for the Athena/X-IFU Instrument
- Author
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Marcel L. Ridder, Emanuele Taralli, J. R. Gao, Pourya Khosropanah, M. P. Bruijn, K. Nagayoshi, S. Visser, Hiroki Akamatsu, and Luciano Gottardi
- Subjects
Superconductivity ,X-IFU ,Fabrication ,Materials science ,business.industry ,Frequency band ,Detector ,Condensed Matter Physics ,01 natural sciences ,Multiplexing ,Aspect ratio (image) ,Atomic and Molecular Physics, and Optics ,010305 fluids & plasmas ,X-ray ,Observatory ,0103 physical sciences ,Optoelectronics ,General Materials Science ,Athena ,Transition edge sensor ,010306 general physics ,business - Abstract
We are developing a transition edge sensor (TES) microcalorimeter array based on a Ti/Au superconducting bilayer, as a backup option for the X-IFU instrument on the Athena X-ray observatory. The array is read out by a frequency-division multiplexing readout system using a 1–5 MHz frequency band. Extensive research collaborations between NASA/Goddard and SRON have led to new design rules for microcalorimeters such as low resistivity of the superconductor bilayer, moderately high ohmic resistance of the TES by changing the aspect ratio and no extra metal strips. We have improved our detector fabrication process according to these design principles and produced TES arrays. Although single-pixel characterizations of these arrays are ongoing, the best energy resolution of 2.0 eV for 5.9 keV X-ray has been observed with a 120 × 20 μm2 TES with a normal resistance of 150 mΩ, biased at 2.2 MHz frequency. This shows that our Ti/Au TES array has a potential to fulfill the detector requirements of the X-IFU instrument.
- Published
- 2019
28. Performance and uniformity of a kilo-pixel array of Ti/Au transition-edge sensor microcalorimeters
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D. Vaccaro, Marcel L. Ridder, M. D'Andrea, Hiroki Akamatsu, Kenichiro Nagayoshi, Luciano Gottardi, Jian-Rong Gao, M. de Wit, Emanuele Taralli, and Marcel P. Bruijn
- Subjects
010302 applied physics ,Physics ,Physics - Instrumentation and Detectors ,Spectrometer ,Physics::Instrumentation and Detectors ,business.industry ,Detector ,FOS: Physical sciences ,Instrumentation and Detectors (physics.ins-det) ,Photon energy ,01 natural sciences ,Noise (electronics) ,010305 fluids & plasmas ,Full width at half maximum ,Optics ,0103 physical sciences ,Spectral resolution ,Transition edge sensor ,Astrophysics - Instrumentation and Methods for Astrophysics ,business ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Instrumentation ,Energy (signal processing) - Abstract
Uniform large transition-edge sensor (TES) arrays are fundamental for the next generation of X-ray space observatories. These arrays are required to achieve an energy resolution $\Delta E$ < 3 eV full-width-half-maximum (FWHM) in the soft X-ray energy range. We are currently developing X-ray microcalorimeter arrays for use in future laboratory and space-based X-ray astrophysics experiments and ground-based spectrometers. In this contribution we report on the development and the characterization of a uniform 32$\times$32 pixel array with 140$\times$30 $\mu$m$^2$ Ti/Au TESs with Au X-ray absorber. We report upon extensive measurements on 60 pixels in order to show the uniformity of our large TES array. The averaged critical temperature is $T_\mathrm{c}$ = 89.5$\pm$0.5 mK and the variation across the array ($\sim$1 cm) is less than 1.5 mK. We found a large region of detector's bias points between 20\% and 40\% of the normal-state resistance where the energy resolution is constantly lower than 3 eV. In particular, results show a summed X-ray spectral resolution $\Delta E_\mathrm{FWHM}$ = 2.50$\pm$0.04 eV at a photon energy of 5.9 keV, measured in a single-pixel mode using a frequency domain multiplexing (FDM) readout system developed at SRON/VTT at bias frequencies ranging from 1 to 5 MHz. Moreover we compare the logarithmic resistance sensitivity with respect to temperature and current ($\alpha$ and $\beta$ respectively) and their correlation with the detector's noise parameter $M$, showing an homogeneous behaviour for all the measured pixels in the array.
- Published
- 2021
29. Low-noise microwave SQUID multiplexed readout of 38 x-ray transition-edge sensor microcalorimeters
- Author
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Marcel L. Ridder, Fuminori Hirayama, Kazuhisa Mitsuda, R. Hayakawa, Luciano Gottardi, Hiroki Akamatsu, J. W. den Herder, Yuki Nakashima, Shinya Yamada, Emanuele Taralli, Noriko Y. Yamasaki, Satoshi Kohjiro, Shuichi Nagasawa, Akira Sato, J. R. Gao, M. P. Bruijn, K. Nagayoshi, and H. Yamamori
- Subjects
010302 applied physics ,Physics ,Physics and Astronomy (miscellaneous) ,business.industry ,02 engineering and technology ,021001 nanoscience & nanotechnology ,01 natural sciences ,Multiplexer ,Noise (electronics) ,law.invention ,SQUID ,Optics ,Sampling (signal processing) ,law ,Magnetic flux quantum ,Rise time ,0103 physical sciences ,Transition edge sensor ,0210 nano-technology ,business ,Microwave - Abstract
We report very-low-noise, fast-response, middle-scale multiplexing in a microwave superconducting quantum interference device multiplexer (MW-Mux) as a transition-edge sensor (TES) readout. Our MW-Mux is able to read 40 channels with 500 kHz sampling and has a low readout noise of 0.9 μ Φ 0 / Hz (where Φ 0 is the magnetic flux quantum), equivalent to 9 pA / Hz. By contrast, a multiplexer of less than 10 pixels with 500 kHz sampling and ∼ 2 μ Φ 0 / Hz readout noise has so far been reported in the literature. Owing to the 500 kHz sampling, our MW-Mux exhibits a fast response to detect a TES pulse with a rise time around 12 μ s. We demonstrated simultaneous readout of 38 pixels from an array of x-ray TES microcalorimeters. The measured full-width values at half-maximum spectral resolution ranged from 2.79 to 4.56 eV, with a median value of 3.30 eV at 5.9 keV, including a ∼ 10 % contribution of readout noise, i.e., 0.9–1.7 eV.
- Published
- 2020
30. The focal plane assembly for the ATHENA x-ray integral field unit instrument (Conference Presentation)
- Author
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Bert-Joost van Leeuwen, M. P. Bruijn, Jan van der Kuur, James A. Chervenak, P. Peille, Jan-Willem den Herder, Brian Jackson, Mikko Kiviranta, Luigi Piro, Johannes Dercksen, Claudio Macculi, Dennis van Loon, Marco Barbera, Hiroki Akamatsu, Didier Barret, Roland H. den Hartog, Caroline A. Kilbourne, Henk van Weers, Flavio Gatti, Luciano Gottardi, Ruud W. M. Hoogeveen, Jean-Michel Mesnager, Francoise Douchin, Stephen J. Smith, Simon R. Bandler, A. Argan, and Hervé Geoffray
- Subjects
Physics ,Cryostat ,Physics::Instrumentation and Detectors ,business.industry ,Detector ,Astrophysics::Instrumentation and Methods for Astrophysics ,Cardinal point ,Optics ,Sensor array ,Observatory ,Electromagnetic shielding ,Spectral resolution ,Transition edge sensor ,business - Abstract
The X-ray Integral Field Unit (X-IFU) is an imaging microcalorimeter being developed for ESA's Athena X-ray observatory to providing high spectral resolution imaging between 0.2-12 keV, with moderate count-rate capability and a large field-of-view. The X-IFU focal plane assembly (FPA) will contain the instrument's large-format transition edge sensor (TES) microcalorimeter array and its superconducting readout electronics, plus a second TES detector, located behind the main sensor array, is used to detect high-energy cosmic rays and secondary particles passing through the sensor array and enable the rejection of false events that they generate in the sensor array's event list. A Kevlar thermal suspension is used to isolate the detectors at 55 mK from the 2 K environment of the X-IFU instrument cryostat's cold stage, while three layers of shielding are used to allow the detector's to achieve their low-noise performance in the expected on-ground and in-flight electromagnetic and microvibration environment. This paper will describe the preliminary design concept of the X-IFU focal plane assembly and its critical technology building blocks.
- Published
- 2018
31. Development of frequency domain multiplexing for the x-ray Integral Field Unit (X-IFU) (Conference Presentation)
- Author
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M. P. Bruijn, A. J. van den Linden, C. P. de Vries, Mikko Kiviranta, Brian Jackson, Jay Chervenak, Nicholas A. Wakeham, Luciano Gottardi, J. van der Kuur, Kazuhiro Sakai, Antoine R. Miniussi, Samuel Smith, and Hiroki Akamatsu
- Subjects
Physics ,Pixel ,Physics::Instrumentation and Detectors ,business.industry ,Amplifier ,Detector ,Astrophysics::Instrumentation and Methods for Astrophysics ,LC circuit ,Multiplexing ,Resonator ,Cardinal point ,Optics ,Spectral resolution ,business - Abstract
We are developing the frequency domain multiplexing (FDM) read-out of transition-edge sensor (TES) microcalorimeters for the X-ray Integral Field Unit (X-IFU) instrument on board of the future European X-Ray observatory Athena. The X-IFU instrument consists of an array of $\sim$3840 TESs with a high quantum efficiency (>90 % at 7 keV) and spectral resolution $\Delta E$=2.5 eV @ 7 keV ($E/\DeltaE\sim$2800). FDM is the baseline readout system for the X-IFU instrument. In FDM, TESs are coupled to a passive LC filter and biased with alternating current (AC bias) at MHz frequencies. Each resonator should be separated beyond their detector thermal response (< 10 kHz) to avoid crosstalk between neighboring resonators. To satisfy the requirement of the X-IFU, a multiplexing factor of 40 pixels/channel in a frequency range from 1 to 5 MHz required. Using high-quality factor LC filters and room temperature electronics developed at SRON and low-noise two-stage SQUID amplifiers provided by VTT, we have recently demonstrated good performance with the FDM readout of Mo/Au TES calorimeters with Au/Bi absorbers. We have achieved a performance requested for the demonstration model (DM) with the single pixel AC bias mode. We have also demonstrated 6-pixel multiplexing with an average energy resolution of 3.4 eV, which is currently limited by non-fundamental issues related to FDM readout in our current lab setup. In parallel to technology developments, we are also constructing a set-up which can be readout 2x40 pixels as the precursor of the DM. In this paper we report on the concept of the focal plane assembly, their requirements, detector performance under FDM scheme, recent results from pre-demonstration model setup and future prospect.
- Published
- 2018
32. Proximity effect model for x-ray Transition Edge Sensors
- Author
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D. J. Goldie, Pourya Khosropanah, Luciano Gottardi, R. C. Harwin, J. R. Gao, and Stafford Withington
- Subjects
Superconductivity ,Materials science ,Transition temperature ,FOS: Physical sciences ,Mechanical engineering ,02 engineering and technology ,021001 nanoscience & nanotechnology ,01 natural sciences ,Superconducting detectors ,Usadel Equations ,0103 physical sciences ,Proximity effect (audio) ,Transition Edge Sensors ,Thin film ,Transition edge sensor ,010306 general physics ,0210 nano-technology ,Astrophysics - Instrumentation and Methods for Astrophysics ,Long Range Proximity Effect ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Transition edge ,S-S'-S Junctions - Abstract
Transition Edge Sensors are ultra-sensitive superconducting detectors with applications in many areas of research, including astrophysics. The device consists of a superconducting thin film, often with additional normal metal features, held close to its transition temperature and connected to two superconducting leads of a higher transition temperature. There is currently no way to reliably assess the performance of a particular device geometry or material composition without making and testing the device. We have developed a proximity effect model based on the Usadel equations to predict the effects of device geometry and material composition on sensor performance. The model is successful in reproducing I −V curves for two devices currently under study. We use the model to suggest the optimal size and geometry for TESs, considering how small the devices can be made before their performance is compromised. In the future, device modelling prior to manufacture will reduce the need for time-consuming and expensive testing.
- Published
- 2018
33. Development of TiAu TES x-ray calorimeters for the X-IFU on ATHENA space observatory
- Author
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Emanuele Taralli, Marcel L. Ridder, Luciano Gottardi, J. R. Gao, K. Nagayoshi, M. P. Bruijn, Pourya Khosropanah, Hiroki Akamatsu, and C. P. de Vries
- Subjects
Physics ,Superconductivity ,Physics::Instrumentation and Detectors ,business.industry ,Resolution (electron density) ,Detector ,Astrophysics::Instrumentation and Methods for Astrophysics ,X-ray ,02 engineering and technology ,021001 nanoscience & nanotechnology ,01 natural sciences ,7. Clean energy ,Noise (electronics) ,Calorimeter ,Thermal conductivity ,Optics ,0103 physical sciences ,Transition edge sensor ,010306 general physics ,0210 nano-technology ,business - Abstract
SRON is developing X-ray transition edge sensor (TES) calorimeters arrays, as a backup technology for X-IFU instrument on the ATHENA space observatory. These detectors are based on a superconducting TiAu bilayer TES with critical temperature of 100 mK on a 1 μm thick SiN membrane with Au or Au/Bi absorbers. Number of devices have been fabricated and measured using a Frequency Division Multiplexing (FDM) readout system with 1-5 MHz bias frequencies. We measured IV curves, critical temperature, thermal conductance, noise and also X-ray energy resolution at number of selected bias points. So far our best calorimeter shows 3.9 eV X-ray resolution at 6 keV. Here we present a summary of our results and the latest status of development of X-ray calorimeters at SRON.
- Published
- 2018
- Full Text
- View/download PDF
34. Developments of Frequency-Domain Multiplexing of TES Arrays for a Future X-Ray Satellite Mission
- Author
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Megan E. Eckart, Luciano Gottardi, R. L. Kelley, Jay Chervenak, Caroline A. Kilbourne, John E. Sadleir, Edward J. Wassell, M. P. Bruijn, Simon R. Bandler, J. W. den Herder, R. den Hartog, Stephen J. Smith, F. M. Finkbeiner, J. van der Kuur, A. J. van den Linden, F. S. Porter, Hiroki Akamatsu, M. Jambunathan, Mikko Kiviranta, Joseph S. Adams, H. F. C. Hoevers, and Sang Jun Lee
- Subjects
Physics ,Cryostat ,Physics::Instrumentation and Detectors ,business.industry ,Amplifier ,Detector ,Astrophysics::Instrumentation and Methods for Astrophysics ,Condensed Matter Physics ,Multiplexing ,Electronic, Optical and Magnetic Materials ,Resonator ,Nuclear magnetic resonance ,Optoelectronics ,Quantum efficiency ,Electrical and Electronic Engineering ,business ,Energy (signal processing) ,Voltage - Abstract
Arrays of transition-edge sensors (TESs) X-ray microcalorimeters can provide high energy resolution and a large area necessary for the future X-ray mission Athena (2028~). An array with 4000 TESs will be employed on the X-ray satellite for the first time. The detector can achieve energy resolution of 2.5-3.0 eV and a high quantum efficiency in the energy range of 0.3-12 keV. Multiplexing the readout is necessary to minimize the number of readout amplifiers, the amount of wiring in the cryostat, and the cooling power required at the base-temperature. We are developing frequency-domain multiplexing (FDM) readout of TES microcalorimeters. In the FDM configuration, the TES is ac voltage biased at well-defined frequencies (between 2 and 6 MHz). For the development of the readout of the Athena instrument, we are using a nearly quantum-limited high-dynamic-range two-stage superconducting quantum interference device amplifier from VTT and high-Q lithographical LC resonators. In this paper, we will present the current status of the development of FDM readout of TES microcalorimeters. We will report on the results obtained using arrays fabricated at the NASA/Goddard Space Flight Center group.
- Published
- 2015
35. Nearly Quantum Limited Two-Stage SQUID Amplifiers for the Frequency Domain Multiplexing of TES Based X-ray and Infrared Detectors
- Author
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M. P. Bruijn, R. den Hartog, Luciano Gottardi, J. van der Kuur, Mikko Kiviranta, and Hiroki Akamatsu
- Subjects
Physics ,Squid ,biology ,business.industry ,Amplifier ,Detector ,Bolometer ,Condensed Matter Physics ,Noise (electronics) ,Electronic, Optical and Magnetic Materials ,law.invention ,Inductance ,Resonator ,law ,biology.animal ,Optoelectronics ,Electrical and Electronic Engineering ,business ,Energy (signal processing) - Abstract
The frequency domain multiplexing (FDM) readout of arrays of transition edges sensors for the X-IFU/Athena and SAFARI/SPICA instruments requires SQUID amplifiers with low input inductance, low flux noise, high-dynamic range and low power consumption. We report the performance of two-stage SQUID amplifiers developed at VTT coupled to multiple high-Q LC resonators of the SRON FDM readout operating in the frequency range from 2 to 5 MHz. The SQUIDs have been tested in the following configurations: 1) the two SQUIDs at base temperature with open input; 2) the amplifier SQUID at 1K temperature and the front-end SQUID at base temperature in the FDM readout of low-G TES bolometers; and 3) and in the FDM readout of X-ray microcalorimeter arrays with both SQUIDS at base temperature. We measured an input flux noise equal to 0.18 μΦ 0 /Hz 1/2 at 20 mK, equivalent to an energy resolution of 9 b. The measured current noise at the SQUID input is ~1 pA/Hz 1/2 at 20 mK, which corresponds to a coupled energy resolution of about 15 b.
- Published
- 2015
36. Thermal Load Minimization of the Frequency Domain Multiplexed Readout for the Athenar X-IFU Instrument
- Author
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B. J. van Leeuwen, Luciano Gottardi, R. den Hartog, B. D. Jackson, H. Akamatsu, Mikko Kiviranta, and J. van der Kuur
- Subjects
Physics::Instrumentation and Detectors ,Computer science ,02 engineering and technology ,microcalorimeter ,SQUID ,7. Clean energy ,01 natural sciences ,Multiplexing ,Frequency-division multiplexing ,power ,0103 physical sciences ,Electronic engineering ,Athena ,Electrical and Electronic Engineering ,010306 general physics ,ta216 ,X-IFU ,multiplexing ,ta114 ,ta213 ,Dynamic range ,Amplifier ,Bandwidth (signal processing) ,Detector ,Astrophysics::Instrumentation and Methods for Astrophysics ,OtaNano ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,Electronic, Optical and Magnetic Materials ,Frequency domain ,Systems design ,0210 nano-technology ,TES - Abstract
The high sensitivity of cryogenic TES-based detectors opens new windows for astrophysical observations ranging from (far) infrared to X-rays. A number of operational and future space and ground-based instruments rely on cryogenic detectors to improve their performance with respect to the capabilities of earlier technologies. To reach the required sensitivities, base temperatures as low as 50 mK are necessary, and stringent requirements on magnetic shielding, microvibrations, and temperature stability are applicable. To minimize the heat load and complexity of the instruments, efficient multiplexing schemes and low-power amplifiers are needed. In addition, for space-based cryogenic instruments, mechanical launch loads and power consumption limitations constrain the available parameter space for engineering further. This paper discusses the system design considerations which are applicable to optimize the multiplex factor within the boundary conditions as set by the space craft for the X-IFU instrument on the Athena observatory. More specifically, the interplay between the science requirements such as pixel dynamic range, pixel speed, and cross talk, and the space craft requirements such as the power dissipation budget, and available bandwidth will be discussed.
- Published
- 2017
37. Transition-edge sensor pixel parameter design of the microcalorimeter array for the x-ray integral field unit on Athena
- Author
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Simon R. Bandler, Brian Jackson, Christine G. Pappas, C. N. Reintsema, Joseph W. Fowler, Meng P. Chiao, Kazuhiro Sakai, Caroline A. Kilbourne, Wonsik Yoon, Joel N. Ullom, Hiroki Akamatsu, F. M. Finkbeiner, Didier Barret, John E. Sadleir, J. van der Kuur, Jay Chervenak, Daniel S. Swetz, Douglas A. Bennett, Megan E. Eckart, Luciano Gottardi, R. L. Kelley, N. Wakeham, Gabriele L. Betancourt-Martinez, R. den Hartog, William B. Doriese, Edward J. Wassell, Joseph S. Adams, A. R. Miniussi, F. S. Porter, Kent D. Irwin, Kelsey M. Morgan, Samuel Smith, Gene C. Hilton, and P. Peille
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010302 applied physics ,Physics ,Pixel ,business.industry ,Point source ,Detector ,Context (language use) ,Large format ,01 natural sciences ,Optics ,Cardinal point ,Hybrid array ,0103 physical sciences ,Transition edge sensor ,010306 general physics ,business - Abstract
The focal plane of the X-ray integral field unit (X-IFU) for ESA's Athena X-ray observatory will consist of approximately 4000 transition edge sensor (TES) x-ray microcalorimeters optimized for the energy range of 0.2 to 12 kiloelectronvolts. The instrument will provide unprecedented spectral resolution of approximately 2.5 electronvolts at energies of up to 7 kiloelectronvolts and will accommodate photon fluxes of 1 milliCrab (90 counts per second) for point source observations. The baseline configuration is a uniform large pixel array (LPA) of 4.28 arcseconds pixels that is read out using frequency domain multiplexing (FDM). However, an alternative configuration under study incorporates an 18 by × 18 small pixel array (SPA) of 2 arcseconds pixels in the central approximately 36 arcseconds region. This hybrid array configuration could be designed to accommodate higher fluxes of up to 10 milliCrabs (900 counts per second) or alternately for improved spectral performance (less than 1.5 electronvolts) at low count-rates. In this paper we report on the TES pixel designs that are being optimized to meet these proposed LPA and SPA configurations. In particular we describe details of how important TES parameters are chosen to meet the specific mission criteria such as energy resolution, count-rate and quantum efficiency, and highlight performance trade-offs between designs. The basis of the pixel parameter selection is discussed in the context of existing TES arrays that are being developed for solar and x-ray astronomy applications. We describe the latest results on DC biased diagnostic arrays as well as large format kilo-pixel arrays and discuss the technical challenges associated with integrating different array types on to a single detector die.
- Published
- 2016
38. The focal plane assembly for the Athena X-ray Integral Field Unit instrument
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L. Piro, Flavio Gatti, M. P. Bruijn, A. Argan, Luciano Gottardi, B. J. van Leeuwen, Mikko Kiviranta, Jay Chervenak, Claudio Macculi, H. van Weers, Hiroki Akamatsu, Didier Barret, Caroline A. Kilbourne, Samuel Smith, Marco Barbera, Thien Lam-Trong, Simon R. Bandler, R. den Hartog, J. W. den Herder, D. Haas, Johannes Dercksen, J. van der Kuur, Brian Jackson, Jackson, B., van Weers, H., van der Kuur, J., den Hartog, R., Akamatsu, H., Argan, A., Bandler, S., Barbera, M., Barret, D., Bruijn, M., Chervenak, J., Dercksen, J., Gatti, F., Gottardi, L., Haas, D., den Herder, J., Kilbourne, C., Kiviranta, M., Lam Trong, T., van Leeuwen, B., Macculi, C., Piro, L., and Smith, S.
- Subjects
Cryostat ,Physics::Instrumentation and Detectors ,Aperture ,01 natural sciences ,frequency division multiplexing ,focal plane assembly ,Settore FIS/05 - Astronomia E Astrofisica ,Optics ,Sensor array ,0103 physical sciences ,Electronic ,SQUID amplifier ,Athena ,Optical and Magnetic Materials ,Electrical and Electronic Engineering ,ta216 ,010306 general physics ,ta113 ,010302 applied physics ,Physics ,X-IFU ,ta114 ,ta213 ,business.industry ,Stray light ,Applied Mathematics ,transition edge sensor ,Detector ,Astrophysics::Instrumentation and Methods for Astrophysics ,X-ray microcalorimeter ,Computer Science Applications1707 Computer Vision and Pattern Recognition ,Condensed Matter Physics ,Cardinal point ,Electromagnetic shielding ,cryogenic anti-coincidence detector ,X-ray microcalorimeter, transition edge sensor, cryogenic anti-coincidence detector, SQUID amplifier, frequency division multiplexing, Athena, X-IFU, focal plane assembly ,Transition edge sensor ,business ,Electronic, Optical and Magnetic Materials - Abstract
This paper summarizes a preliminary design concept for the focal plane assembly of the X-ray Integral Field Unit on the Athena spacecraft, an imaging microcalorimeter that will enable high spectral resolution imaging and point-source spectroscopy. The instrument's sensor array will be a ~ 3840-pixel transition edge sensor (TES) microcalorimeter array, with a frequency domain multiplexed SQUID readout system allowing this large-format sensor array to be operated within the thermal constraints of the instrument's cryogenic system. A second TES detector will be operated in close proximity to the sensor array to detect cosmic rays and secondary particles passing through the sensor array for off-line coincidence detection to identify and reject events caused by the in-orbit high-energy particle background. The detectors, operating at 55 mK, or less, will be thermally isolated from the instrument cryostat's 2 K stage, while shielding and filtering within the FPA will allow the instrument's sensitive sensor array to be operated in the expected environment during both on-ground testing and in-flight operation, including straylight from the cryostat environment, low-energy photons entering through the X-ray aperture, low-frequency magnetic fields, and high-frequency electric fields.
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- 2016
39. Optimising the multiplex factor of the frequency domain multiplexed readout of the TES-based microcalorimeter imaging array for the X-IFU instrument on the Athena x-ray observatory
- Author
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B. J. Jackson, Mikko Kiviranta, H. Akamatsu, B. J. van Leeuwen, R. den Hartog, D. Haas, J. van der Kuur, Luciano Gottardi, den Herder, Jan-Willem, Takahashi, Tadayuki, and Bautz, Marshall
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Physics - Instrumentation and Detectors ,Physics::Instrumentation and Detectors ,FOS: Physical sciences ,Field of view ,02 engineering and technology ,Spica ,7. Clean energy ,01 natural sciences ,Multiplexing ,law.invention ,Optics ,law ,Observatory ,0103 physical sciences ,Athena ,ta216 ,010306 general physics ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,ta113 ,Physics ,X-IFU ,ta114 ,ta213 ,Spectrometer ,Pixel ,business.industry ,Bolometer ,Detector ,Astrophysics::Instrumentation and Methods for Astrophysics ,Instrumentation and Detectors (physics.ins-det) ,OtaNano ,021001 nanoscience & nanotechnology ,frequency domain multiplexing ,readout ,Astrophysics - Instrumentation and Methods for Astrophysics ,0210 nano-technology ,business ,TES - Abstract
Athena is a space-based X-ray observatory intended for exploration of the hot and energetic universe. One of the science instruments on Athena will be the X-ray Integrated Field Unit (X-IFU), which is a cryogenic X-ray spectrometer, based on a large cryogenic imaging array of Transition Edge Sensors (TES) based microcalorimeters operating at a temperature of 100mK. The imaging array consists of 3800 pixels providing 2.5 eV spectral resolution, and covers a field of view with a diameter of of 5 arc minutes. Multiplexed readout of the cryogenic microcalorimeter array is essential to comply with the cooling power and complexity constraints on a space craft. Frequency domain multiplexing has been under development for the readout of TES-based detectors for this purpose, not only for the X-IFU detector arrays but also for TES-based bolometer arrays for the Safari instrument of the Japanese SPICA observatory. This paper discusses the design considerations which are applicable to optimise the multiplex factor within the boundary conditions as set by the space craft. More specifically, the interplay between the science requirements such as pixel dynamic range, pixel speed, and cross talk, and the space craft requirements such as the power dissipation budget, available bandwidth, and electromagnetic compatibility will be discussed.
- Published
- 2016
40. Ultra-low noise TES bolometer arrays for SAFARI instrument on SPICA
- Author
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Pourya Khosropanah, R. A. Hijmering, J. R. Gao, Luciano Gottardi, Toyoaki Suzuki, Marcel L. Ridder, Hiroki Akamatsu, J. van der Kuur, and Brian Jackson
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Superconductivity ,Physics ,Photon ,SPICA ,business.industry ,Phonon ,Bolometer ,SAFARI ,Spica ,01 natural sciences ,law.invention ,TES arrays ,SiN membrane ,Optics ,Etching (microfabrication) ,law ,0103 physical sciences ,Far infrared spectrometer ,Optoelectronics ,010306 general physics ,business ,Phonon noise ,Transition edge sensor ,010303 astronomy & astrophysics ,Noise (radio) - Abstract
SRON is developing ultra-low noise Transition Edge Sensors (TESs) based on a superconducting Ti/Au bilayer on a suspended SiN island with SiN legs for the SAFARI instrument aboard the SPICA mission. We successfully fabricated TESs with very narrow (0.5-0.7 μm) and thin (0.25 μm) SiN legs on different sizes of SiN islands using deep reactiveion etching process. The pixel size is 840x840 μm2 and there are variety of designs with and without optical absorbers. For TESs without absorbers, we measured electrical NEPs as low as -19 W/√Hz with response time of 0.3 ms and reached the phonon noise limit. Using TESs with absorbers, we quantified the darkness of our setup and confirmed a photon noise level of 2x10-19 W/√Hz.
- Published
- 2016
41. Microcalorimeter pulse analysis by means of principle component decomposition
- Author
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Luciano Gottardi, R. M. Schouten, C. P. de Vries, J. van der Kuur, and Hiroki Akamatsu
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Photon ,Field (physics) ,Computer science ,FOS: Physical sciences ,01 natural sciences ,Multiplexing ,010305 fluids & plasmas ,Set (abstract data type) ,Frequency domain ,0103 physical sciences ,Principal component analysis ,Transition edge sensor ,010306 general physics ,Astrophysics - Instrumentation and Methods for Astrophysics ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Algorithm ,Energy (signal processing) - Abstract
The X-ray integral field unit for the Athena mission consists of a microcalorimeter transition edge sensor pixel array. Incoming photons generate pulses which are analyzed in terms of energy, in order to assemble the X-ray spectrum. Usually this is done by means of optimal filtering in either time or frequency domain. In this paper we investigate an alternative method by means of principle component analysis. This method attempts to find the main components of an orthogonal set of functions to describe the data. We show, based on simulations, what the influence of various instrumental effects is on this type of analysis. We compare analyses both in time and frequency domain. Finally we apply these analyses on real data, obtained via frequency domain multiplexing readout., SPIE Astronomical Telescopes and Instrumentation; conference contribution
- Published
- 2016
42. TES-Based X-ray Microcalorimeter Performances Under AC Bias and FDM for Athena
- Author
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Pourya Khosropanah, Megan E. Eckart, Luciano Gottardi, J. R. Gao, J. W. den Herder, K. Ravensberg, F. M. Finkbeiner, Edward J. Wassell, Toyoaki Suzuki, Simon R. Bandler, Samuel Smith, M. P. Bruijn, Jay Chervenak, J. van der Kuur, Sang Jun Lee, R. E. Kelley, John E. Sadleir, A. J. van den Linden, H. F. C. Hoevers, Caroline A. Kilbourne, Joseph S. Adams, F. S. Porter, Mikko Kiviranta, R. den Hartog, Hiroki Akamatsu, and C. P. de Vries
- Subjects
Physics::Instrumentation and Detectors ,Astrophysics::High Energy Astrophysical Phenomena ,Imaging spectrometer ,Astrophysics::Cosmology and Extragalactic Astrophysics ,01 natural sciences ,Multiplexing ,Frequency-division multiplexing ,Optics ,Observatory ,Frequency domain multiplexing ,0103 physical sciences ,General Materials Science ,Athena ,010306 general physics ,010302 applied physics ,Physics ,business.industry ,Transition edge sensors ,Detector ,Astrophysics::Instrumentation and Methods for Astrophysics ,X-ray microcalorimeter ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,Calorimeter ,Transition edge sensor ,business ,Energy (signal processing) - Abstract
Athena is a European X-ray observatory, scheduled for launch in $$\sim $$ 2028. Athena will employ a high-resolution imaging spectrometer called X-ray integral field unit (X-IFU), consisting of an array of $$\sim $$ 4000 transition edge sensor (TES) microcalorimeter pixels. For the readout of X-IFU, we are developing frequency domain multiplexing, which is the baseline readout system. In this paper, we report on the performance of a TES X-ray calorimeter array fabricated at Goddard Space Flight Center (GSFC) at MHz frequencies for the baseline of X-IFU detector. During single-pixel AC bias characterization, we measured X-ray energy resolutions (at 6 keV) of about 2.9 eV at both 2.3 and 3.7 MHz. Furthermore, in the multiplexing mode, we measured X-ray energy resolutions of about 2.9 eV at 1.3 and 1.7 MHz.
- Published
- 2016
43. Development of the superconducting detectors and read-out for the X-IFU instrument on board of the X-ray observatory Athena
- Author
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J. W. den Herder, M. P. Bruijn, Luciano Gottardi, H. van Weers, Hiroki Akamatsu, Brian Jackson, R. den Hartog, J. van der Kuur, and Mikko Kiviranta
- Subjects
Nuclear and High Energy Physics ,Physics - Instrumentation and Detectors ,Physics::Instrumentation and Detectors ,Astrophysics::High Energy Astrophysical Phenomena ,FOS: Physical sciences ,Astrophysics ,01 natural sciences ,law.invention ,Telescope ,Superconductivity (cond-mat.supr-con) ,Optics ,law ,Observatory ,Frequency domain multiplexing ,0103 physical sciences ,010306 general physics ,Instrumentation ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,010302 applied physics ,Physics ,X-IFU ,Spectrometer ,business.industry ,Condensed Matter - Superconductivity ,Detector ,Bandwidth (signal processing) ,Astrophysics::Instrumentation and Methods for Astrophysics ,Instrumentation and Detectors (physics.ins-det) ,Measuring instrument ,Quantum efficiency ,Transition edge sensor ,business ,Astrophysics - Instrumentation and Methods for Astrophysics ,Athena mission - Abstract
The Advanced Telescope for High-Energy Astrophysics (Athena) has been selected by ESA as its second large-class mission. The future European X-ray observatory will study the hot and energetic Universe with its launch foreseen in 2028. Microcalorimeters based on superconducting Transition-edge sensor (TES) are the chosen technology for the detectors array of the X-ray Integral Field Unit (X-IFU) on board of Athena. The X-IFU is a 2-D imaging integral-field spectrometer operating in the soft X-ray band (0.3 -12 keV). The detector consists of an array of 3840 TESs coupled to X-ray absorbers and read out in the MHz bandwidth using Frequency Domain Multiplexing (FDM) based on Superconducting QUantum Interference Devices (SQUIDs). The proposed design calls for devices with a high filling-factor, high quantum efficiency, relatively high count-rate capability and an energy resolution of 2.5 eV at 5.9 keV. The paper will review the basic principle and the physics of the TES-based microcalorimeters and present the state-of-the art of the FDM read-out., 4 pages,4 figures, available on line (http://www.sciencedirect.com/science/article/pii/S0168900215011274)
- Published
- 2016
44. Study of the dependency on magnetic field and bias voltage of an AC-biased TES microcalorimeter
- Author
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Roland den Hartog, Richard L. Kelley, Mark A. Lindeman, Frank Finkbeiner, C. N. Bailey, Jack Sadleir, Marcel P. Bruijn, Jan van der Kuur, Megan E. Eckart, Steve Smith, Luciano Gottardi, Simon R. Bandler, James A. Chervenak, Caroline A. Kilbourne, Frederick S. Porter, James B. Adams, Henk F.C. Hoevers, and Piet A. J. de Korte
- Subjects
Superconductivity ,Physics ,Photon ,Condensed matter physics ,Physics::Instrumentation and Detectors ,Condensed Matter - Superconductivity ,Detector ,FOS: Physical sciences ,Biasing ,x-ray detector ,Condensed Matter Physics ,SQUID ,Noise (electronics) ,Atomic and Molecular Physics, and Optics ,Article ,LC resonator ,Computational physics ,Magnetic field ,Superconductivity (cond-mat.supr-con) ,Full width at half maximum ,Materials Science(all) ,rf-SQUID ,General Materials Science ,TES ,Energy (signal processing) - Abstract
At SRON we are studying the performance of a Goddard Space Flight Center single pixel TES microcalorimeter operated in an AC bias configuration. For x-ray photons at 6 keV the pixel shows an x-ray energy resolution $dE_{FWHM} = 3.7\mathrm{eV}$, which is about a factor 2 worse than the energy resolution observed in an identical DC-biased pixel. In order to better understand the reasons for this discrepancy we characterised the detector as a function of temperature, bias working point and applied perpendicular magnetic field. A strong periodic dependency of the detector noise on the TES AC bias voltage is measured. We discuss the results in the framework of the recently observed weak-link behaviour of a TES microcalorimeter, Comment: 6 pages, 5 figures
- Published
- 2016
- Full Text
- View/download PDF
45. AC bias characterization of low noise bolometers for SAFARI using an Open-Loop Frequency Domain SQUID-based multiplexer operating between 1 and 5 MHz
- Author
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Mark A. Lindeman, M. Ridder, Marcel P. Bruijn, J. van der Kuur, Henk F.C. Hoevers, Luciano Gottardi, R. den Hartog, J. R. Gao, R A Hijmering, P. Khosropanah, and P. A. J. de Korte
- Subjects
Physics - Instrumentation and Detectors ,FOS: Physical sciences ,Spica ,Multiplexer ,law.invention ,Superconductivity (cond-mat.supr-con) ,Resonator ,Materials Science(all) ,law ,General Materials Science ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Physics ,Spectrometer ,business.industry ,Condensed Matter - Superconductivity ,Amplifier ,Bolometer ,Instrumentation and Detectors (physics.ins-det) ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,SQUID ,Frequency domain ,Optoelectronics ,FDM · Infra-red detector · SQUID · Bolometer · TES · LC resonator ,Astrophysics - Instrumentation and Methods for Astrophysics ,business - Abstract
SRON is developing the Frequency Domain Multiplexing (FDM) readout and the ultra low NEP TES bolometers array for the infrared spectrometer SAFARI on board of the Japanese space mission SPICA. The FDM prototype of the instrument requires critical and complex optimizations. For single pixel characterization under AC bias we are developing a simple FDM system working in the frequency range from 1 to 5 MHz, based on the open loop read-out of a linearized two-stage SQUID amplifier and high Q lithographic LC resonators. We describe the details of the experimental set-up required to achieve low power loading (< 1 fW) and low noise (NEP $\sim 10^{-19} W/Hz^{1/2}$) in the TES bolometers. We conclude the paper by comparing the performance of a $4 \cdot 10^{-19} W/Hz^{1/2}$ TES bolometer measured under DC and AC bias., 6 pages, 5 figures
- Published
- 2016
- Full Text
- View/download PDF
46. Josephson effects in an alternating current biased transition edge sensor
- Author
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A. G. Kozorezov, Roland den Hartog, Anton J. van der Linden, Jan van der Kuur, Marcel L. Ridder, Toyo Suzuki, Luciano Gottardi, Jan R. Gao, Pourya Khosropanah, R. A. Hijmering, Colin J. Lambert, Marcel P. Bruijn, and Hiroki Akamatsu
- Subjects
Josephson effect ,Physics ,Superconductivity ,Physics - Instrumentation and Detectors ,Physics and Astronomy (miscellaneous) ,Condensed matter physics ,Condensed Matter - Superconductivity ,FOS: Physical sciences ,Biasing ,Instrumentation and Detectors (physics.ins-det) ,Noise (electronics) ,law.invention ,Superconductivity (cond-mat.supr-con) ,law ,Condensed Matter::Superconductivity ,Transition edge sensor ,Alternating current ,Electrical impedance ,Voltage - Abstract
We report the experimental evidence of the ac Josephson effect in a transition edge sensor (TES) operating in a frequency domain multiplexer and biased by ac voltage at MHz frequencies. The effect is observed by measuring the non-linear impedance of the sensor. The TES is treated as a weakly linked superconducting system and within the resistively shunted junction model framework. We provide a full theoretical explanation of the results by finding the analytic solution of the non-inertial Langevian equation of the system and calculating the non-linear response of the detector to a large ac bias current in the presence of noise., Comment: 4 pages, 4 figures
- Published
- 2016
- Full Text
- View/download PDF
47. Development of frequency domain multiplexing for the X-ray Integral Field unit (X-IFU) on the Athena
- Author
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Marcel P. Bruijn, J. S. Adams, Cor P. de Vries, A. J. van der Linden, Simon R. Bandler, Mikko Kiviranta, Stephen J. Smith, K. Ravensberg, Jan van der Kuur, Hiroki Akamatsu, Caroline A. Kilbourne, James A. Chervenak, Brian Jackson, and Luciano Gottardi
- Subjects
TESs ,FOS: Physical sciences ,7. Clean energy ,01 natural sciences ,Multiplexing ,010305 fluids & plasmas ,law.invention ,Frequency-division multiplexing ,Optics ,law ,X-ray Integral Field Unit (X-IFU) ,0103 physical sciences ,Athena ,Spectral resolution ,010306 general physics ,ta216 ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Noise-equivalent power ,Physics ,ta113 ,Pixel ,ta114 ,ta213 ,business.industry ,Amplifier ,X-ray microcalorimeter ,OtaNano ,frequency domain multiplexing (FDM) read-out ,SQUID ,Transition edge sensor ,business ,Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
We are developing the frequency domain multiplexing (FDM) read-out of transition-edge sensor (TES) microcalorimeters for the X-ray Integral Field Unit (X-IFU) instrument on board of the future European X-Ray observatory Athena. The X-IFU instrument consists of an array of $\sim$3840 TESs with a high quantum efficiency ($>$90 \%) and spectral resolution $\Delta E$=2.5 eV $@$ 7 keV ($E/\Delta E\sim$2800). FDM is currently the baseline readout system for the X-IFU instrument. Using high quality factor LC filters and room temperature electronics developed at SRON and low-noise two stage SQUID amplifiers provided by VTT, we have recently demonstrated good performance with the FDM readout of Mo/Au TES calorimeters with Au/Bi absorbers. An integrated noise equivalent power resolution of about 2.0 eV at 1.7 MHz has been demonstrated with a pixel from a new TES array from NASA/Goddard (GSFC-A2). We have achieved X-ray energy resolutions $\sim$2.5 eV at AC bias frequency at 1.7 MHz in the single pixel read-out. We have also demonstrated for the first time an X-ray energy resolution around 3.0 eV in a 6 pixel FDM read-out with TES array (GSFC-A1). In this paper we report on the single pixel performance of these microcalorimeters under MHz AC bias, and further results of the performance of these pixels under FDM., Comment: 8 pages, 4 figures, Proceedings of the SPIE Astronomical Instrumentation "Space Telescopes and Instrumentation 2014: Ultraviolet to Gamma Ray"
- Published
- 2016
48. Distributed TES Model for Designing Low Noise Bolometers Approaching SAFARI Instrument Requirements
- Author
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R. A. Hijmering, Luciano Gottardi, Pourya Khosropanah, H. F. C. Hoevers, P. A. J. de Korte, M. P. Bruijn, Marcel L. Ridder, M. A. Lindeman, J. van der Kuur, and J. R. Gao
- Subjects
Physics ,business.industry ,Detector ,Bolometer ,transition edge sensor · TES · far infrared spectrometer · submm spectrometer · SiN membrane · cryogenic detectors · THz detectors ,Imaging spectrometer ,Spica ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,Low noise ,law.invention ,Telescope ,Optics ,Materials Science(all) ,law ,Thermal ,General Materials Science ,Transition edge sensor ,business - Abstract
Transition edge sensors (TES) are the chosen detector technology for the SAFARI imaging spectrometer on the SPICA telescope. The TES are required to have an NEP of 2–3 × 10?19 W/? Hz to take full advantage of the cooled mirror. SRON has developed TiAu TES bolometers for the short wavelength band (30–60 ?m). The TES are on SiN membranes, in which long and narrow legs act as thermal links between the TES and the bath. We present a distributed model that accounts for the heat conductance and the heat capacity in the long legs that provides a guideline for designing low noise detectors. We report our latest results that include a measured dark NEP of 4.2×10?19 W/? Hz and a saturation power of about 10 fW.
- Published
- 2012
49. Carrier Phase Optimization for Frequency Division Multiplexing of Low Temperature Detectors
- Author
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R. A. Hijmering, Luciano Gottardi, M. A. Lindeman, H. F. C. Hoevers, Pourya Khosropanah, P. A. J. de Korte, Roland H. den Hartog, and J. van der Kuur
- Subjects
Physics ,Carrier signal ,Carrier phase ,business.industry ,Detector ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,Frequency-division multiplexing ,Sine wave ,Amplitude ,Optoelectronics ,General Materials Science ,Electronics ,Crest factor ,business - Abstract
A large number of low temperature detectors may be read out via few wires using frequency division multiplexing. In this scheme, each detector is biased by a sine wave with a unique carrier frequency. Numerous carriers can be combined in a single pair of wires. However, the combined signals occasionally result in large peak amplitudes in the bias or the readout. This stresses the capabilities of the electronics. We developed an efficient algorithm to optimize the phases and frequencies of the carriers in order to obtain a low crest factor. We also find that more regularly spaced carrier frequencies result in a lower crest factor, compared to irregularly spaced carriers.
- Published
- 2012
50. High-Q LC Filters for FDM Read out of Cryogenic Sensor Arrays
- Author
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M. P. Bruijn, Luciano Gottardi, Mikko Kiviranta, H. F. C. Hoevers, R. den Hartog, J. van der Kuur, and P. A. J. de Korte
- Subjects
Physics ,Superconductivity ,H [a-Si] ,business.industry ,a-Si:H ,Close-packing of equal spheres ,superconducting resonators ,multiplexed read-out ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,Resonator ,Quality (physics) ,cryogenic detectors ,SPICA-SAFARI ,Superconducting resonators ,Optoelectronics ,General Materials Science ,Planar coil ,Center frequency ,business - Abstract
We present new results on the development of larger arrays (presently 72 channels, goal of multiple units of 160 channels) of superconducting LC filters. The a-Si:H based resonators show a quality factor above 10.000. The latest design utilizes oppositely wound planar coil pairs which enable close packing with low magnetic cross talk. We present results on the obtained center frequency distribution within the range of 1 to 3 MHz.
- Published
- 2011
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