Jose Lorenzo Alvarez
European Space Agency
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Featured researches published by Jose Lorenzo Alvarez.
International Symposium on Optical Science and Technology | 2001
Jose Lorenzo Alvarez; Maikel Hernandez; Pablo Benitez; Juan Carlos Minano
In this work it is presented a new design of a TIR lens-mushrooms lens device developed with the Simultaneous Multiple Surfaces (SMS) method. In SMS nomenclature, it is named TIR-R. In contrast to previous TIR-mushroom designs, application of the SMS method to this configuration consists in the simultaneous design of both TIR (total internal reflection) and R (refraction) optical surfaces using extended ray-bundles and the edge-ray theorem. In this paper is presented a basic approach to do the design. In this basic approach, first it is considered the TIR lens as a microstructured surface with infinitesimal flat facets. Afterwards, it is generated a TIR lens with finite size facets from the already designed one. In an advanced approach could be considered the TIR lens with finite facet size and designed simultaneously each facet with a portion of the outer surface of the mushroom lens. With respect to others SMS high-gain devices (as the RXI), the TIR-R concentrator has the following advantages: is a mirror-less device, there is not shadowing elements, and the receiver/emitter elements placement is more favorable for encapsulation and electrical connection. As it is common in the SMS devices, the TIR-R concentrator achieves wide acceptance angle and high efficiency with a low aspect ratio (thickness to entry aperture diameter ratio). For example, a 1256X concentration device has a theoretical efficiency of 100 percent (without optical losses) with an acceptance angle of +/- 1.7 decgrees, and an aspect ratio of 0.34.
Optical Science and Technology, SPIE's 48th Annual Meeting | 2004
Pablo Benítez; Juan C. Miñano; José Blen; Rubén Mohedano; Julio Chaves; Oliver Dross; Maikel Hernandez; Jose Lorenzo Alvarez; Waqidi Falicoff
The Simultaneous Multiple Surface (SMS) method in 3D geometry is presented. Giving two orthotomic input ray bundles and other two orthotomic output ray bundles, the method provides an optical system with two free-form surfaces that deflects the rays of the input bundles into the rays of the corresponding output bundles and vice versa. In nonimaging applications, the method allows controlling the light emitted by an extended light source much better than single free-form surfaces designs, and also enables the optics contour to be shaped without efficiency losses. The method is expected to find also applications in imaging optics
Proceedings of SPIE | 2016
Giuseppe D. Racca; R. J. Laureijs; Luca Stagnaro; Jean-Christophe Salvignol; Jose Lorenzo Alvarez; Gonzalo Saavedra Criado; Luis Gaspar Venancio; Alex Short; Paolo Strada; Tobias Bönke; Cyril Colombo; Adriano Calvi; Elena Maiorano; Osvaldo Piersanti; Sylvain Prezelus; Pierluigi Rosato; Jacques Pinel; Hans Rozemeijer; Valentina Lesna; Paolo Musi; Marco Sias; Alberto Anselmi; Vincent Cazaubiel; Ludovic Vaillon; Y. Mellier; Jérôme Amiaux; Michel Berthé; Marc Sauvage; Ruyman Azzollini; Mark Cropper
Euclid is a space-based optical/near-infrared survey mission of the European Space Agency (ESA) to investigate the nature of dark energy, dark matter and gravity by observing the geometry of the Universe and on the formation of structures over cosmological timescales. Euclid will use two probes of the signature of dark matter and energy: Weak gravitational Lensing, which requires the measurement of the shape and photometric redshifts of distant galaxies, and Galaxy Clustering, based on the measurement of the 3-dimensional distribution of galaxies through their spectroscopic redshifts. The mission is scheduled for launch in 2020 and is designed for 6 years of nominal survey operations. The Euclid Spacecraft is composed of a Service Module and a Payload Module. The Service Module comprises all the conventional spacecraft subsystems, the instruments warm electronics units, the sun shield and the solar arrays. In particular the Service Module provides the extremely challenging pointing accuracy required by the scientific objectives. The Payload Module consists of a 1.2 m three-mirror Korsch type telescope and of two instruments, the visible imager and the near-infrared spectro-photometer, both covering a large common field-of-view enabling to survey more than 35% of the entire sky. All sensor data are downlinked using K-band transmission and processed by a dedicated ground segment for science data processing. The Euclid data and catalogues will be made available to the public at the ESA Science Data Centre.
Proceedings of SPIE | 2008
Tanya Lim; Jose Lorenzo Alvarez; Eva Bauwens; Alejandro Garcia Bedregal; Joris Blommaert; H. Dannerbauer; Paul Eccleston; Marc Ferlet; Sebastian Fischer; M. García-Marín; Alistair Glasse; Adrian M. Glauser; Karl D. Gordon; Tom Greene; Tim Grundy; Martin Hennemann; Ulrich Klaas; A. Labiano; F. Lahuis; J. R. Martínez-Galarza; Bruno Merin Martin; J. E. Morrison; Theodoros Nakos; Brian O'Sullivan; Bart Pindor; Michael E. Ressler; Bryan Shaughnessy; B. Vandenbussche; Martyn Wells; G. Wright
The Mid-Infrared Instrument (MIRI) is one of the three scientific instruments to fly on the James Webb Space Telescope (JWST), which is due for launch in 2013. MIRI contains two sub-instruments, an imager, which has low resolution spectroscopy and coronagraphic capabilities in addition to imaging, and a medium resolution IFU spectrometer. A verification model of MIRI was assembled in 2007 and a cold test campaign was conducted between November 2007 and February 2008. This model was the first scientifically representative model, allowing a first assessment to be made of the performance. This paper describes the test facility and testing done. It also reports on the first results from this test campaign.
Optical Engineering | 2000
Rube´n Mohedano; Juan C. Min˜ano; Pablo Benı´tez; Jose Lorenzo Alvarez; Maikel Herna´ndez; Juan C. Gonza´lez; Kazutoshi Hirohashi; Satoru Toguchi
Advanced optical design methods using the tools of nonimaging optics (instead of conventional imaging tools) produce ultracompact devices that combine high collection efficiency with a concentration (or collimating) capability close to the thermodynamic limit. After a general overview covering the most important design methods and devices in nonimaging optics, two of these designs, the so-called RX and RXI, are presented. Even though it is designed within the nonimaging framework, the RX device nevertheless has imaging properties that complement its valuable performance as a nonimaging device. The RXI is extremely compact: its aspect ratio (thickness/aperture diameter) is less than 1/3. When working as a receiver, that is, by placing a photodiode in the correct position, it attains an increase in irradiance that takes it beyond 95% of the theoretical thermodynamic limit (i.e., a concentration of 1600 times with an acceptance angle of ±2.14 deg). As an emitter, similar intensity gains can be obtained within an angle almost as large as 95% of the thermodynamic limit. The combination of high concentration factors, relatively wide acceptance angles, simplicity, and compactness makes these devices almost unique. The measurements carried out with several RXI prototypes, all of them made by PMMA injection, are also presented.
Proceedings of SPIE | 1999
Juan C. Miñano; Pablo Benítez; Ruben Mohedano Arroyo; Jose Lorenzo Alvarez; Maikel Hernandez; Juan-Carlos Gonzalez; Kazutoshi Hirohashi; Satoru Toguchi
Advanced optical design methods using the keys of nonimaging optics lead to some ultra compact designs which combine the concentrating (or collimating) capabilities of conventional long focal length systems with a high collection efficiency. One of those designs is the so-called RXI. Its aspect ratio (thickness/aperture diameter) is less than 1/3. Used as a receiver, i.e. placing a photodiode at the proper position, it gets an irradiance concentration of the 95% of the theoretical thermodynamic limit (this means for example, a concentration of 1600 times with an acceptance angle of +/- 2.14 degrees). When used as an emitter (replacing the aforementioned photodiode by an LED, for instance), similar intensity gains may be obtained within an angle cone almost as wide as the 95% of the thermodynamic limit. In a real device these irradiance(and intensity)gains are reduced by the optical efficiency. This combination of high concentration factors, relatively wide angles, simplicity and compactness make the optical device almost unique. This work will show the results of the measurements done with several RXI prototypes of 40-mm aperture diameter, all of them made of PMMA (by injection process).
Proceedings of SPIE | 2016
Luis M. Gaspar Venancio; Charlotte Pachot; Lionel Carminati; Jose Lorenzo Alvarez; Jérôme Amiaux; Eric Prieto; Luciana Bonino; Jean-Christophe Salvignol; Alex Short; Tobias Boenke; Paulo Strada; R. J. Laureijs
In the Euclid mission the straylight has been identified at an early stage as the main driver for the final imaging quality of the telescope. The assessment by simulation of the final straylight in the focal plane of both instruments in Euclid’s payload have required a complex workflow involving all stakeholders in the mission, from industry to the scientific community. The straylight is defined as a Normalized Detector Irradiance (NDI) which is a convenient definition tool to separate the contributions of the telescope and of the instruments. The end-to-end straylight of the payload is then simply the sum of the NDIs of the telescope and of each instrument. The NDIs for both instruments are presented in this paper for photometry and spectrometry.
Proceedings of SPIE | 2007
Maurice te Plate; Jose Lorenzo Alvarez; Pierre-Antoine Frugier; Pierangelo Marenaci
The James Webb Space Telescope (JWST) Observatory, the follow-on mission to the Hubble Space Telescope, will yield astonishing breakthroughs in infrared space science. One of the four instruments on that mission, the NIRSpec instrument, is being developed by the European Space Agency with EADS Astrium Germany GmbH as the prime contractor. This multi-object spectrograph is capable of measuring the near infrared spectrum of at least 100 objects simultaneously at various spectral resolutions in the 0.6 μm to 5.0 μm wavelength range. A physical optical model, based on Fourier Optics, was developed in order to simulate some of the key optical performances of NIRSpec. Realistic WFE maps were established for both the JWST optical telescope as well as for the various NIRSpec optical stages. The model simulates the optical performance of NIRSpec at the key optical pupil and image planes. Using this core optical simulation module, the model was expanded to a full instrument performance simulator that can be used to simulate the response of NIRSpec to any given optical input. The program will be of great use during the planning and evaluation of performance testing and calibration measurements.
Proceedings of SPIE | 2016
Luis M. Gaspar Venancio; Lionel Carminati; Jose Lorenzo Alvarez; Jérôme Amiaux; Luciana Bonino; Jean-Christophe Salvignol; Roland Vavrek; R. J. Laureijs; Alex Short; Tobias Boenke; Paulo Strada
The challenging constraints imposed on the Euclid telescope imaging performances have driven the design, manufacturing and characterisation of the multi-layers coatings of the dichroic. Indeed it was found that the coatings layers thickness inhomogeneity will introduce a wavelength dependent phase-shift resulting in degradation of the image quality of the telescope. Such changes must be characterized and/or simulated since they could be non-negligible contributors to the scientific performance accuracy. Several papers on this topic can be found in literature, however the results can not be applied directly to Euclid’s dichroic coatings. In particular an applicable model of the phase-shift variation with the wavelength could not be found and was developed. The results achieved with the mathematical model are compared to experimental results of tests performed on a development prototype of the Euclid’s dichroic.
Proceedings of SPIE | 2016
Roland Vavrek; R. J. Laureijs; Jose Lorenzo Alvarez; Jérôme Amiaux; Y. Mellier; Ruyman Azzollini; Guillermo Buenadicha; Gonzalo Saavedra Criado; Mark Cropper; Christophe Dabin; A. Ealet; Bianca Garilli; Anna Gregorio; Henk Hoekstra; Knud Jahnke; Martin Kilbinger; Tom Kitching; John Hoar; Will J. Percival; Giuseppe Racca; Jean Christophe Salvignol; Marc Sauvage; R. Scaramella; Luis M. Gaspar Venancio; Yun Wang; A. Zacchei; Stefanie Wachter
ESAs Dark Energy Mission Euclid will map the 3D matter distribution in our Universe using two Dark Energy probes: Weak Lensing (WL) and Galaxy Clustering (GC). The extreme accuracy required for both probes can only be achieved by observing from space in order to limit all observational biases in the measurements of the tracer galaxies. Weak Lensing requires an extremely high precision measurement of galaxy shapes realised with the Visual Imager (VIS) as well as photometric redshift measurements using near-infrared photometry provided by the Near Infrared Spectrometer Photometer (NISP). Galaxy Clustering requires accurate redshifts (Δz/(z+1)<0.1%) of galaxies to be obtained by the NISP Spectrometer. Performance requirements on spacecraft, telescope assembly, scientific instruments and the ground data-processing have been carefully budgeted to meet the demanding top level science requirements. As part of the mission development, the verification of scientific performances needs mission-level end-to-end analyses in which the Euclid systems are modeled from as-designed to final as-built flight configurations. We present the plan to carry out end-to-end analysis coordinated by the ESA project team with the collaboration of the Euclid Consortium. The plan includes the definition of key performance parameters and their process of verification, the input and output identification and the management of applicable mission configurations in the parameter database.