Título Calibrating LISA Pathfinder raw data into femto-g differential accelerometry
Autores Vetrugno, Daniele , Karnesis, Nikolaos , Armano, M. , Audley, H. , Auger, G. , Baird, J. , Bassan, M. , Binetruy, P. , Born, M. , Bortoluzzi, D. , Brandt, N. , Caleno, M. , Cavalleri, A. , Cesarini, A. , Cruise, M. , Danzmann, K. , de Deus Silva, M. , De Rosa, R. , Di Fiore, L. , Diepholz, I. , Dolesi, R. , Dunbar, N. , Ferraioli, L. , Ferroni, V. , Fitzsimons, E. , Flatscher, R. , Freschi, M. , Marrirodriga, C. Garcia , Gerndt, R. , Gesa, L. , Gibert, F. , Giardini, D. , Giusteri, R. , Grado, A. , Grimani, C. , Grzymisch, J. , Harrison, I. , Heinzel, G. , Hewitson, M. , Hollington, D. , Hoyland, D. , Hueller, M. , Inchauspe, H. , Jennrich, O. , Jetzer, P. , Johlander, B. , Karnesis, N. , Kaune, B. , Korsakova, N. , Killow, C. , Lobo, A. , Lloro, I. , Liu, L. , Lopez-Zaragoza, J. P. , Maarschalkerweerd, R. , Mance, D. , Martin, V. , Martin-Polo, L. , Martino, J. , Martin-Porqueras, F. , Madden, S. , Mateos, I. , McNamara, P. W. , Mendes, J. , Mendel, L. , Nofrarias, M. , Paczkowski, S. , Perreur-Lloyd, M. , Petiteau, A. , Pivato, P. , Plagnol, E. , Prat, P. , Ragnit, U. , Ramos-Castro, J. , Reiche, J. , Robertson, D. I. , Rozemeijer, H. , RIVAS GARCÍA, FRANCISCO, Russano, G. , Sarra, P. , Schleicher, A. , Shaul, D. , Slutsky, J. , Sopuerta, C. F. , Stanga, R. , Sumner, T. , Texier, D. , Thorpe, J. I. , Trenke, C. , Troebs, M. , Vetrugno, D. , Vitale, S. , Wanner, G. , Ward, H. , Wass, P. , Wealthy, D. , Weber, W. J. , Wissel, L. , Wittchen, A. , Zambotti, A. , Zanoni, C. , Ziegler, T. , Zweifel, P. , LPF Collaboration
Publicación externa Si
Medio J. Phys. Conf. Ser.
Alcance Proceedings Paper
Naturaleza Científica
Cuartil SJR 3
Impacto SJR 0.24100
Fecha de publicacion 01/01/2017
ISI 000437968700002
DOI 10.1088/1742-6596/840/1/012002
Abstract LISA Pathfinder is an in-flight test of the local sources of acceleration noise in LISA. The acceleration noise level in LISA Pathfinder is measured by the residual differential acceleration Delta g between the two test masses once the coupling to the spacecraft motion has been removed. The full process from raw data to Delta g passes through a series of calibration experiments and different data elaboration procedure which are thoroughly used during the mission and represent the baseline for any other further investigation.
Miembros de la Universidad Loyola

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