5 results on '"Rodriguez Castillo, S."'
Search Results
2. Metal 3D printing for RF/microwave high-frequency parts
- Author
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Martín-Iglesias, P., Marechal, M., Calves, P., Hazard, M., Pambaguian, L., Brandao, A., Rodriguez Castillo, S., Martin, T., Percaz, J., Iza, V., Martín-Iglesias, S., Arregui, I., Teberio, F., Lopetegi, T., Laso, M. A. G., Martin, Thierry, Immunologie et chimie thérapeutiques (ICT), Cancéropôle du Grand Est-Centre National de la Recherche Scientifique (CNRS), Institut de biologie moléculaire et cellulaire (IBMC), Université de Strasbourg (UNISTRA)-Centre National de la Recherche Scientifique (CNRS), Institut de Génétique et de Biologie Moléculaire et Cellulaire (IGBMC), Université de Strasbourg (UNISTRA)-Institut National de la Santé et de la Recherche Médicale (INSERM)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique Théorique - UMR 7332 (CPT), Aix Marseille Université (AMU)-Université de Toulon (UTLN)-Centre National de la Recherche Scientifique (CNRS), Aix Marseille Université (AMU), Université de Strasbourg (UNISTRA), Immuno-Rhumatologie Moléculaire, Université de Strasbourg (UNISTRA)-Institut National de la Santé et de la Recherche Médicale (INSERM), Logiques de l'Agir ( UR 2274) (LdA), Université de Franche-Comté (UFC), Université Bourgogne Franche-Comté [COMUE] (UBFC)-Université Bourgogne Franche-Comté [COMUE] (UBFC), CHU Strasbourg, Les Hôpitaux Universitaires de Strasbourg (HUS), Centre National d'Études Spatiales [Toulouse] (CNES), European Synchroton Radiation Facility [Grenoble] (ESRF), Nouvel Hôpital Civil de Strasbourg, CPT - E6 Nanophysique, Aix Marseille Université (AMU)-Université de Toulon (UTLN)-Centre National de la Recherche Scientifique (CNRS)-Aix Marseille Université (AMU)-Université de Toulon (UTLN)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Génie des Procédés et Matériaux (LGPM), CentraleSupélec-Université Paris-Saclay, Universidad Pública de Navarra. Departamento de Ingeniería Eléctrica, Electrónica y de Comunicación, and Nafarroako Unibertsitate Publikoa. Ingeniaritza Elektriko, Elektroniko eta Telekomunikazio Saila
- Subjects
manufacturing ,[SPI.ELEC]Engineering Sciences [physics]/Electromagnetism ,microwave ,e antennas ,Space and Planetary Science ,Waveguide ,Aerospace Engineering ,Antennas ,space ,3D printing ,waveguid - Abstract
Space Systems have been historically characterised by high performance, high reliability and high cost. Every new generation of space systems tends to improve performance, keep as much as possible reliability, speeding the lead time and lower the cost. Aggressive approach is nowadays followed by some of the players of the new space ecosystem where, for instance, reli- ability can be relaxed thanks for the in-orbit redundancy or robustness to failures by having a constellation with a high number of satellites. This push towards the technology and system limit requires to investigate new methods for the manufacturing of RF/Microwave parts. RF devices such as those based on waveguide structures, benefit from an additive manufacturing approach in terms of radio frequency (RF) performance and compactness. However each manufacturing approach comes with specific features and limitations which need to be well understood and, in some cases, even taking advantage of them. This paper provides a short review of some of the RF/Microwave parts already manufactured using this technology. The paper will focus mainly on metal 3D printing parts since this technology is, at the moment, well accepted by the space community. UPNA thanks the support of the Spanish Ministerio de Ciencia e Innovación-Agencia Estatal de Investigación (MCIN/AEI/ 10.13039/501100011033) under Project PID2020-112545RB-C53.
- Published
- 2022
- Full Text
- View/download PDF
3. Astrochemical relevance of VUV ionization of large PAH cations
- Author
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Wenzel, G., primary, Joblin, C., additional, Giuliani, A., additional, Rodriguez Castillo, S., additional, Mulas, G., additional, Ji, M., additional, Sabbah, H., additional, Quiroga, S., additional, Peña, D., additional, and Nahon, L., additional
- Published
- 2020
- Full Text
- View/download PDF
4. Photo-processing of astro-PAHs
- Author
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Joblin, C, primary, Wenzel, G, additional, Rodriguez Castillo, S, additional, Simon, A, additional, Sabbah, H, additional, Bonnamy, A, additional, Toublanc, D, additional, Mulas, G, additional, Ji, M, additional, Giuliani, A, additional, and Nahon, L, additional
- Published
- 2020
- Full Text
- View/download PDF
5. Unimolecular reaction energies for polycyclic aromatic hydrocarbon ions.
- Author
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West B, Rodriguez Castillo S, Sit A, Mohamad S, Lowe B, Joblin C, Bodi A, and Mayer PM
- Abstract
Imaging photoelectron photoion coincidence spectroscopy was employed to explore the unimolecular dissociation of the ionized polycyclic aromatic hydrocarbons (PAHs) acenaphthylene, fluorene, cyclopenta[d,e,f]phenanthrene, pyrene, perylene, fluoranthene, dibenzo[a,e]pyrene, dibenzo[a,l]pyrene, coronene and corannulene. The primary reaction is always hydrogen atom loss, with the smaller species also exhibiting loss of C
2 H2 to varying extents. Combined with previous work on smaller PAH ions, trends in the reaction energies (E0 ) for loss of H from sp2 -C and sp3 -C centres, along with hydrocarbon molecule loss were found as a function of the number of carbon atoms in the ionized PAHs ranging in size from naphthalene to coronene. In the case of molecules which possessed at least one sp3 -C centre, the activation energy for the loss of an H atom from this site was 2.34 eV, with the exception of cyclopenta[d,e,f]phenanthrene (CPP) ions, for which the E0 was 3.44 ± 0.86 eV due to steric constraints. The hydrogen loss from PAH cations and from their H-loss fragments exhibits two trends, depending on the number of unpaired electrons. For the loss of the first hydrogen atom, the energy is consistently ca. 4.40 eV, while the threshold to lose the second hydrogen atom is much lower at ca. 3.16 eV. The only exception was for the dibenzo[a,l]pyrene cation, which has a unique structure due to steric constraints, resulting in a low H loss reaction energy of 2.85 eV. If C2 H2 is lost directly from the precursor cation, the energy required for this dissociation is 4.16 eV. No other fragmentation channels were observed over a large enough sample set for trends to be extrapolated, though data on CH3 and C4 H2 loss obtained in previous studies is included for completeness. The dissociation reactions were also studied by collision induced dissociation after ionization by atmospheric pressure chemical ionization. When modeled with a simple temperature-based theory for the post-collision internal energy distribution, there was reasonable agreement between the two sets of data.- Published
- 2018
- Full Text
- View/download PDF
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