23–25 oct. 2018
Institut d'Astrophysique de Paris
Fuseau horaire Europe/Paris

Liste des Contributions

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  1. Philippe Brax (IPHT Saclay)
    23/10/2018 10:30
  2. Christophe Yeche (CEA Irfu/SPP)
    23/10/2018 11:10
  3. Frederic Henry-Couannier
    23/10/2018 11:50
  4. Xavier Sarazin (LAL), François COUCHOT (CNRS/IN2P3/LAL)
    23/10/2018 12:10
  5. Valeria Pettorino (CEA Paris-Saclay, Departement of Astrophysics, CosmoStat Lab)
    23/10/2018 14:00
  6. Alejandro Perez (LPNHE), Dr Daniel Sudarsky (UNAM), Prof. James D. Bjorken (SLAC )
    23/10/2018 14:40
  7. Maxim Khlopov (APC and MEPHI)
    23/10/2018 15:00
  8. Dominique Boutigny (LAPP)
    23/10/2018 15:20
  9. Stéphane Ilic (Institut de Recherche en Astrophysique et Planétologie)
    23/10/2018 16:30
  10. Fabien Lacasa (Université de Genève)
    23/10/2018 16:50
  11. Dr Emille Ishida (LPC-UCA)
    23/10/2018 17:10
  12. Eric Jullo (LAM)
    23/10/2018 17:50
  13. Dr Emmanuel Bertin (IAP)
    24/10/2018 09:00
  14. Marguerite PIERRE (CEA Saclay)
    24/10/2018 09:40
  15. Cecile Renault (LPSC)
    24/10/2018 10:20
  16. Prof. Nick Kaiser (ENS)
    24/10/2018 11:10
  17. Aurelien Hees (SYRTE - Observatoire de Paris), Dr Michel Abgrall (SYRTE, Observatoire de Paris), Dr Sebastien Bize (SYRTE, Observatoire de Paris), Dr Pacome Delva (SYRTE, Observatoire de Paris), Dr Jocelyne Guéna (SYRTE, Observatoire de Paris), Dr Olivier Minazzoli (Artemis, OCA and CSM), Dr Benjamin Roberts (SYRTE, Observatoire de Paris), Dr Etienne Savalle (SYRTE, Observatoire de Paris), Yevgeny Stadnik (Johannes Gutenberg University of Mainz)
    24/10/2018 11:50
  18. Ixandra Achitouv
    24/10/2018 12:10
  19. Dr Edward Porter (APC Paris)
    24/10/2018 14:00
  20. Adrien Kuntz (CPT Marseille)
    24/10/2018 14:40
  21. Christian Marinoni (Centre de Physique Théorique, Marseille)
    24/10/2018 15:00
  22. Filippo Vernizzi (IPhT - CEA Saclay)
    24/10/2018 15:20
  23. Karim Noui (LMPT Tours)
    24/10/2018 16:00
  24. Dr Yann Rasera (LUTH)
    24/10/2018 16:50
  25. Pierros Ntelis (Astroparticule et Cosmology Group)
    24/10/2018 17:30
  26. Sylvain de la Torre (LAM)
    24/10/2018 17:50
  27. 24/10/2018 19:40
  28. Emmanuel Gangler (LPC)
    25/10/2018 09:00
  29. Johanna Pasquet (CPPM)
    25/10/2018 09:40
  30. Dr Agnes Ferte (Jet Propulsion Laboratory)
    25/10/2018 10:00
  31. Mickael Rigault (LPC)
    25/10/2018 10:20
  32. Agnes FIENGA (Institut UTINAM)
    25/10/2018 11:10
  33. Pierre-François Léget (Stanford University)
    25/10/2018 12:00
  34. Alain Blanchard (IRAP , OMP), Stéphane Ilic (Institut de Recherche en Astrophysique et Planétologie), ziad sakr (IRAP : Institut de Recherche en Astrophysique et Planétologie)
    25/10/2018 12:20
  35. Dr Ziad Sakr (IRAP : Institut de Recherche en Astrophysique et Planétologie)
    25/10/2018 14:20
  36. Romain Graziani (IPNL)
    25/10/2018 14:40
  37. Guillaume Pignol (LPSC)
    25/10/2018 15:00
  38. M. Françis Bernardeau (IAP)
    25/10/2018 15:20
  39. Alain Blanchard (IRAP , OMP)
    25/10/2018 16:00
  40. Johanna Pasquet (CPPM)

    Future large surveys like the Large Synoptic Survey Telescope (LSST) aim to increase the precision and accuracy of observational cosmology. In particular, LSST will observe a large quantity of well-sampled type Ia supernovae that will be one of the major probe of dark energy. However the spectroscopic follow-up for the identification of supernovae and the estimation of redshift will be...

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  41. Prof. Alejandro Perez (Centre de Physique Theorique)

    We argue that discreteness at the Planck scale (naturally expected to arise from quantum gravity) might manifest in the form of minute violations of energy-momentum conservation of the matter degrees of freedom when described in terms of (idealized) smooth fields on a smooth spacetime. In the context of applications to cosmology such `energy diffusion' from the low energy matter degrees of...

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  42. Dr Aurelien Hees (SYRTE, Observatoire de Paris)

    In several theoretical scenarios, a scalar field is introduced to model dark energy. While some properties of this scalar field can be constrained by cosmological observations, certain properties like its coupling with the standard model fields can be searched for with local experiments such as the ones testing for the universality of free fall and the ones using atomic clocks. Such...

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  43. Stéphane Ilic (Institut de Recherche en Astrophysique et Planétologie)

    Grâce aux mesures de lentillage gravitationnel et de clustering des galaxies, la prochaine génération de grands relevés (Euclid, LSST) posera des contraintes sans précédent sur l'Univers récent. D'autre part, des observations CMB de haute qualité (Planck et futures expérience) sont capables d'imposer des contraintes strictes sur l'Univers primordial. Je montrerai comment la combinaison et la...

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  44. Stéphane Ilic (Institut de Recherche en Astrophysique et Planétologie)
  45. Pierros Ntelis (Astroparticule et Cosmology Group)

    In the era of the upcoming stage IV surveys, the sky will be more revealing than ever. In this talk, I will put the homogeneity scale in the general cosmological context. I will show how one can use the homogeneity scale as a standard ruler to learn about the large scale structures.

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  46. Xavier Sarazin (LAL)

    As initially proposed by H.A. Wilson, then R.H. Dicke, the curved spacetime in a stationary gravitational field can be equivalently interpreted as being due to a spatial change of both the vacuum refractive index and the inertial masses in a Euclidean metric. Dicke further extended this framework to explain the cosmological redshift, assuming a flat and static Euclidean metric but a vacuum...

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  47. Fabien Lacasa (Université de Genève)

    One of the main challenges for cosmological analysis of future galaxy surveys is the non-linearity of the evolution of the large scale structure (LSS). Among the consequences of this non-linearity is the development of non-Gaussianity of the density field. And this non-Gaussianity yields new covariance terms for our observables, additional to the classical Gaussian variance that we have been...

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  48. Christian Marinoni (Centre de Physique Théorique, Marseille)

    High-precision astrometric experiments might constrain our proper acceleration through space via real-time observations of the change in the aberration of sources at cosmic distances.
    The cosmological component of this aberration drift signal, the non-inertial motion generated by the large-scale distribution of matter, can in principle be detected by
    astrometric surveys. It can provide...

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  49. Dr Mickael Rigault (LPC)

    I will present the Hubble Constant controversy, that is, the different direct or indirect measurements of the Hubble Constant and how some are in significant tension. Then I'll present our current work on astrophysical bias in Type Ia Supernova distance measurements and explain how such effect could explain the aforementioned tension.

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  50. Alain BLANCHARD (IRAP , OMP)

    Le modèle LCDM est un succès remarquable de la cosmologie moderne, rendant compte des principales observations du champ cosmologique, ses six paramètres de base étant maintenant mesurés avec une précision de l'ordre du pourcent. L'abondance des amas détectés par effet SZ est toutefois très en deçà des prédictions du modèle normalisé aux fluctuations mesurées par Planck. L'origine de cette...

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  51. Dr Agnes Ferte (Jet Propulsion Laboratory)

    The Dark Energy Survey is one of the largest ongoing survey probing the late universe, specially through galaxy clustering and weak gravitational lensing. The data from the first year of DES observations were used to constrain the LambdaCDM model in 1708.01530, combining clustering and weak lensing measurements from the same experiment for the first time. We used this combination of data to...

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  52. Dr Pierre-François Léget (Stanford University)

    Type Ia Supernova (SNIa) distance measurement for cosmology is based on a well-established observational paradigm that two main effects explain their variabilities in luminosity: stretch (link to intrinsic properties), and color (link mainly to dust extinction). However, after correcting the luminosity of both stretch and color, an intrinsic scatter in luminosity and a correlation of Hubble...

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  53. Adrien Kuntz (CPT Marseille)

    Dans cette présentation, je parlerai de la théorie effective de Goldberger et Rothstein pour obtenir les équations régissant un système binaire. Je montrerai comment elle peut être adaptée à une théorie tenseur-scalaire en mettant en avant les points sur lesquelles ces théories diffèrent de la relativité générale.

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  54. M. Safir Yahia-Cherif (IRAP)

    One of the main prediction of inflationary cosmology is the spatial flatness of the universe. The combination of observed CMB fluctuations with SNIa observations and BAO leads to a prediction of the spatial curvature parameter lower than 1e-4. Observations have shown the acceleration of the expansion of the universe revealing the existence of two dark component : the dark matter and the dark...

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  55. Dr Ixandra Achitouv (Observatoire de Paris )

    The growth rate of cosmic structures is a powerful quantity to probe gravitational interactions and dark energy. In the late-time Universe the growth rate becomes non-linear, making it more difficult to probe, but also makes it in principle a source of additional cosmological information than its linear counterpart. In this talk, I will discuss why it becomes interesting to probe the growth...

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  56. Eric Jullo (LAM)

    The combination of GGL and RSD allow to break the degeneracy between the growth rate parameter $f$ and the matter density $\Omega_m$. In this talk, I will present our results obtained with the BOSS/CMASS sample at redshift $z=0.57$, and the weak-lensing over an area of 338 deg$^2$. Using an ensemble of joint lensing and clustering lightcones, we also characterize the statistical properties of...

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  57. frederic henry-couannier

    Dark Gravity theories are extensions of General Relativity aiming at a stable anti-gravitational sector. The most natural extension of GR in presence of a flat non dynamical background turns out to be such a Dark Gravity theory and it is able to reproduce GR predictions extremely well in many sectors except that it avoids true Black Hole Horizon as well as Big-Bang singularity. The symmetries...

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  58. Dr Ziad SAKR (IRAP - USJ)

    In the frame of the dark energy colloquium, we investigate the impact of a dark energy different from fiducial $\Lambda$CDM, on a discrepancy on the amplitude of matter fluctuation $\sigma_8$ found between local and deep probes. In particular between local, X ray, or near universe, SZ detected cluster counts samples and deep CMB temperature and polarization angular correlation spectrums.
    We...

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  59. Karim Noui (LMPT Tours)

    Les théories tenseur-scalaire offrent un cadre formidable pour tester les éventuelles limites de la relativité générale. Elles sont des modifications de la théorie d'Einstein qui pourraient rendre compte de la présence d'énergie noire dans l'univers par exemple.
    Je vous propose de présenter tout d'abord la construction d'une très grande classe de théories tenseur-scalaire qui a fortement été...

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  60. Prof. Maxim Khlopov (APC and MIFI)

    Taking apart cosmological constant, being constant by definition, physics of dark energy may lead to its time dependence. In the simplest case time dependence of the homogeneously distributed comological energy can be implemented in the model with cosmological term and unstable dark matter, decaying after the first objects are formed and contributing the homogeneously distributed energy...

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