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| DOI | 10.1051/0004-6361/202348691 | ||||
| Año | 2024 | ||||
| Tipo | artículo de investigación |
Citas Totales
Autores Afiliación Chile
Instituciones Chile
% Participación
Internacional
Autores
Afiliación Extranjera
Instituciones
Extranjeras
Context. The use of artificial laser guide stars (LGS) is planned for the new generation of giant segmented mirror telescopes in order to extend the sky coverage of their adaptive optics systems. The LGS, being a 3D object at a finite distance, will have a large elongation that will affect its use with the Shack- Hartmann (SH) wavefront sensor. Aims. In this paper, we compute the expected performance for a Pyramid WaveFront Sensor (PWFS) using an LGS for a 40 m telescope affected by photon noise, and also extend the analysis to a flat 2D object as reference. Methods. We developed a new way to discretize the LGS, and a new, faster method of propagating the light for any Fourier filtering wavefront sensors (FFWFS) when using extended objects. We present the use of a sensitivity model to predict the performance of a closed-loop adaptive optic system. We optimized a point-source-calibrated interaction matrix to accommodate the signal of an extended object by computing optical gains using a convolutional model. Results. We find that the sensitivity drop, given the size of the extended laser source, is large enough to make the system operate in a low-performance regime given the expected return flux of the LGS. The width of the laser beam is identified as the limiting factor, rather than the thickness of the sodium layer. Even an ideal, flat LGS will have a drop in performance due to the flux of the LGS, and small variations in the return flux will result in large variations in performance. Conclusions. We conclude that knife-edge-like wavefront sensors, such as the PWFS, are not recommended for use with LGS for a 40 m telescope, as they will operate in a low-performance regime, given the size of the extended object.
| Ord. | Autor | Género | Institución - País |
|---|---|---|---|
| 1 | Oyarzún, F. | - |
Laboratoire d'Astrophysique de Marseille - Francia
Aix Marseille Univ - Francia |
| 2 | Chambouleyron, V. | - |
University of California, Santa Cruz - Estados Unidos
Univ Calif Santa Cruz - Estados Unidos |
| 3 | Neichel, Benoit | Hombre |
Laboratoire d'Astrophysique de Marseille - Francia
Aix Marseille Univ - Francia |
| 4 | Fusco, T. | Hombre |
Laboratoire d'Astrophysique de Marseille - Francia
Universite Paris-Saclay - Francia Aix Marseille Univ - Francia Univ Paris Saclay - Francia |
| 5 | Guesalaga, A. | Hombre |
Pontificia Universidad Católica de Chile - Chile
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| Fuente |
|---|
| Agence Nationale de la Recherche |
| CNES |
| Centre National de la Recherche Scientifique |
| French National Research Agency (ANR) |
| Centre National d’Etudes Spatiales |
| INSU |
| LabEx FOCUS |
| ECOS-Conycit |
| Action Spécifique Haute Résolution Angulaire |
| Action Specifique Haute Resolution Angulaire (ASHRA) of CNRS/INSU |
| WOLF |
| ECOS-CONYCIT France-Chile cooperation |
| Conseil Régional Provence-Alpes-Côte d'Azur |
| APPLY |
| Programme Investissement Avenir F-CELT |
| Millennium Science Initiative Program (ACIP) |
| ORP-H2020 Framework Programme of the European Commission’s |
| First Light Imaging |
| ORP-H2020 Framework Programme of the European Commissions |
| ORP-H2020 Framework Programme of the European Commission's |
| Conseil regional Provence-Alpes-Cpte d'Azur |
| French government under the France 2030 investment plan, Initiative d'Excellence d'Aix-Marseille Universite A*MIDEX |
| Agradecimiento |
|---|
| This work benefited from the support of the French National Research Agency (ANR) with WOLF (ANR-18-CE31-0018), APPLY (ANR-19-CE31-0011) and LabEx FOCUS (ANR-11-LABX-0013); the Programme Investissement Avenir F-CELT (ANR-21-ESRE-0008), the Action Sp\u00E9cifique Haute R\u00E9solution Angulaire (ASHRA) of CNRS/INSU co-funded by CNES, the ECOS-CONYCIT France-Chile cooperation (C20E02), the ORP-H2020 Framework Programme of the European Commission\u2019s (Grant number 101004719), STIC AmSud (21-STIC-09), the french government under the France 2030 investment plan, as part of the Initiative d\u2019Excellence d\u2019Aix-Marseille Universit\u00E9 A*MIDEX, program number AMX-22-RE-AB-151, the Conseil r\u00E9gional Provence-Alpes-C\u00F4te d\u2019Azur with the emplois jeune doctorant program, co-funded by First Light Imaging, and the Millennium Science Initiative Program (ACIP, NCN19 161). |
| This work benefited from the support of the French National Research Agency (ANR) with WOLF (ANR-18-CE31-0018), APPLY (ANR-19-CE31-0011) and LabEx FOCUS (ANR-11-LABX-0013); the Programme Investissement Avenir F-CELT (ANR-21-ESRE-0008), the Action Sp\u00E9cifique Haute R\u00E9solution Angulaire (ASHRA) of CNRS/INSU co-funded by CNES, the ECOS-CONYCIT France-Chile cooperation (C20E02), the ORP-H2020 Framework Programme of the European Commission\u2019s (Grant number 101004719), STIC AmSud (21-STIC-09), the french government under the France 2030 investment plan, as part of the Initiative d\u2019Excellence d\u2019Aix-Marseille Universit\u00E9 A*MIDEX, program number AMX-22-RE-AB-151, the Conseil r\u00E9gional Provence-Alpes-C\u00F4te d\u2019Azur with the emplois jeune doctorant program, co-funded by First Light Imaging, and the Millennium Science Initiative Program (ACIP, NCN19 161). |
| This work benefited from the support of the French National Research Agency (ANR) with WOLF (ANR-18-CE31-0018), APPLY (ANR-19-CE31-0011) and LabEx FOCUS (ANR-11-LABX-0013); the Programme Investissement Avenir F-CELT (ANR-21-ESRE-0008), the Action Specifique Haute Resolution Angulaire (ASHRA) of CNRS/INSU co-funded by CNES, the ECOS-CONYCIT France-Chile cooperation (C20E02), the ORP-H2020 Framework Programme of the European Commission's (Grant number 101004719), STIC AmSud (21-STIC-09), the French government under the France 2030 investment plan, as part of the Initiative d'Excellence d'Aix-Marseille Universite A*MIDEX, program number AMX-22-RE-AB-151, the Conseil regional Provence-Alpes-Cpte d'Azur with the emplois jeune doctorant program, co-funded by First Light Imaging, and the Millennium Science Initiative Program (ACIP, NCN19 161). |