cosmology with large telescopes
play

Cosmology with Large Telescopes: an ESO-centric view Catherine - PowerPoint PPT Presentation

Cosmology with Large Telescopes: an ESO-centric view Catherine Cesarsky ESO Venice, August 2007 The Very Large Telescope (VLT) The ALMA Project (2012) ELTs: the world scene 2 US projects Giant Magellan Telescope (21-m)


  1. Cosmology with Large Telescopes: an ESO-centric view Catherine Cesarsky ESO Venice, August 2007

  2. The Very Large Telescope (VLT)

  3. The ALMA Project (2012)

  4. ELTs: the world scene • 2 US projects – Giant Magellan Telescope (21-m) • Carnegie & US Universities – Thirty Meter Telescope • Caltech, U. of Calif., Canada GMT TMT

  5. E-ELT • 42m baseline diameter • Innovative 5-mirror design • Excellent image quality 50 mas Axis 1’ 2’ 3’ 4’ 5’ • Reconfigurable: multiple foci F/16 gravity Coude F/15+F/16 invariant

  6. E-ELT Stiff mechanics FE models and analysis 85008 elements 27106 nodes Cross Altitude: 2.1 Hz Altitude locked rotor: 2.5 Hz

  7. E-ELT Powerful built-in AO - M4+M5: GLAO, LTAO - Plus post-focal AO : ExAO, MCAO, MOAO, … M4 AO mirror (adaptive) options WAVEFRONT ABERRATION Waves 1.0000 M5 (tip-tilt) 0.5000 0.0000 Field = ( 0.000,0.0833) Degrees Wavelength = 586.0 nm Defocusing = 0.000000 cm Optical design laser friendly

  8. E-ELT Instrumentation friendly Nasmyth : MCAO module Coude: Codex

  9. Part 1:Fundamental Cosmology • Spectroscopy of distant supernovae • Ly � forest: • small scale coherence length of the mass distribution • variation of physical constants • dynamic measurement of the acceleration of the Universe • Age of the oldest stars

  10. Supernova evidence for acceleration Riess et al. 2004

  11. ESSENCE • World-wide collaboration to find and characterise SNe Ia with 0.2 < z < 0.8 • Search with CTIO 4m Blanco telescope • Spectroscopy with VLT, Gemini, Keck, Magellan • Goal: Measure distances to 200 SNe Ia with an overall accuracy of 5% � determine � to 10% overall

  12. SNLS – The SuperNova Legacy Survey • World-wide collaboration to find and characterise SNe Ia with 0.2 < z < 0.8 • Search with CFHT 4m telescope • Spectroscopy with VLT, Gemini, Keck, Magellan • Goal: Measure distances to 1000 SNe Ia with an overall accuracy of 5% � determine � to 7% overall

  13. First cosmology results published • SNLS – Astier et al. 2006 – 71 distant SNe Ia – various papers describing spectroscopy (Lidman et al. 2006, Hook et al. 2006), rise time (Conley et al. 2006) and individual SNe (Howell et al. 2006) • ESSENCE – Wood-Vasey et al. 2007 – 60 distant SNe Ia – Miknaitis et al. 2007 – description of the survey – Davis et al. 2007 – comparison to exotic dark energy proposals – spectroscopy (Matheson et al. 2005, Blondin et al. 2006)

  14. Time variable w? w=w0+wa (1-a) Distance module versus z Wood-Vasey et al. 2007 Residuals for (-1, 0.27, 0.73) universe

  15. High-z SNe with ELTs: What type of AO? • Use a low-z reference galaxy image shifted to higher z: – angular scale changes – surface brightness changes (+ crude galaxy evolution model) • “Supernova” = point source with approx 80% of galaxy flux • Convolve with different AO PSFs

  16. Simulations for a 42m telescope H band on axis, z=1.65 LTAO MCAO Few (~ 2’ arcsec FOV) GLAO No AO (~5’ PSFs from FOV) Le Louarn et al.

  17. High-z Supernovae with ELT • ELT ideal for high-z spectroscopy – redshifts and types – detailed test of evolution • 42m ELT with AO could reach – z =1.7 (no OH suppression) – or z~4 with OH suppression – using AO GRBs could also be used for similar purposes Statistical Comparison of high and low-z spectral features –Garavini et al.(2007)

  18. Combined analysis of Lyman � forest matter power spectrum, weak lensing and CMB Conclusion: Sigma 8 (co-moving rms of density fluctuations in sphere of radius 8/h Mpc) slightly higher than with WMAP alone Lesgourgues et al.2007 (VHS; Viel et al.2006)

  19. Cosmic structure at small scales Lyman � -forests of two pairs of QSOs observed with UVES; separations: ~ 1’. z ~ 2.6 and 2.1; (B mag : 18.8-20.5) (d’Odorico et al. 2006) With the 2 nd generation VLT instrument X-shooter , higher SNR to fainter magnitudes will make Observations of distant QSO pairs can be used to measure the structure of the intergalactic H I possible to increase significantly and to derive the cosmological parameters. the QSO pair sample Present results fit with the concordance model.

  20. (2008)

  21. Alcock-Paczynski test using the X-shooter (2 nd generation VLT spectrograph) # of QSO pairs (V mag of the faintest one) Expected SNR with Xshooter 2 < z < 3 � z < 0.1 �� < 3’ � < +15° � The transverse distance scale, which is sensitive to the vacuum energy ( � ?) can be determined through the 3-D correlation of Ly � forests of neighboring QSO spectra .An accuracy of 10 % on can be achieved analyzing 13 ( � /1’) � QSO pairs with separation < � (McDonald 2003). � Given the current counts on QSO pairs (left plot) and the performance prediction on the X-shooter the measurement becomes possible with ~140 hr exposure time ( � 120 faint QSOs)

  22. Variability of Physical Constants from QSO Absortion Line Spectra In many models the cosmological evolution of dark energy is accompanied by variations of the fine-structure constant � and of the electron/proton mass ratio � . These variations could be used to trace the evolution with z of the equation of state parameter w From accurate measurements of the absorption line centers in QSO metal absorption lines From Molecular Rotational vs. Vibrational modes of H2 molecules

  23. Measurement of a possible variability of fundamental constants: upper limits of �� from Keck (HIRES) and VLT (UVES) spectra of QSO Very accurate measurements of lines centers of different ion transitions in QSO absorption systems. Status: detection at the limit of accuracy, possibly still biased by systematic errors. Contradictory results from different data sets or the application of different methods. Fig.1 Fig.2 Murphy et al.- fig1 (2004), Chand et al -fig2- (2004)., Levshakov et al (2007)

  24. e.g. Variation of µ = m p /m e Ivanchik et al. (2005, A&A, 440, 45), see also Reinhold et al. (2006), Murphy et al (2006) and many more….. The wavelength of electron-vibro- rotational lines depend on the reduced mass of the molecule Laboratory obs � � µ � � i ( 1 z ) 1 K = + + � � abs i lab � µ � � i Coefficients K have been calculated (Varshalovich and Potekhin 1995) Observations

  25. Profiles of lines selected Q0347-383 Q0405-443 UVES: 20 hours per line of sight Absorptions free of blending and Narrow lines

  26. Correlation between (z-< z>)/(1+<z>) and K? • Systematics ? -> Need for more laboratory wavelength measurements •Increase the number of lines of sight WITH the same absorption lines •Increase S/N ratio

  27. High-Precision Spectrographs at ELTs (e.g. CODEX @ 42m) will be able to increase the accuracy by 2 orders of magnitude (better S/N, special calibration techniques) and give much more significant constraints Reconstruction of equation of state Simulated data set as state-of-art and band of uncertainty (grey area): (upper panels) and with CODEX at dashed line corresponding to input to ELT , for a given DE model , lower simulations, solid line reconstruction’s panels (Martins, 2006) best fit. (Martins, 2006)

  28. Cosmic Dynamics Experiment De- or acceleration of the universal expansion rate causes a small change in observed redshifts as a function of time: Measuring � (z): • Allows us to watch, in real-time, the Universe changing its expansion rate. • Most direct and model- independent route to the expansion history. • First non-geometric measurement of the global RW metric. • Independent confirmation and quantification of accelerated expansion. z & v & Solid lines: Dashed lines: in cm/s

  29. Cosmic Dynamics Experiment Measuring the redshift drift requires: • E-ELT • High resolution, extremely stable spectrograph • ~15 yr long spectroscopic monitoring campaign Best place to observe the redshift drift: the Lyman- � forest.

  30. Cosmic Dynamics Experiment Can we collect enough photons to achieve the required accuracy? Yes: 20 known QSOs with 2 < z < 5 are bright enough to achieve a 3 c m / s radial velocity accuracy 4 cm/s of 3 cm/s with 3200 hours on a 42-m ELT.

  31. Cosmic Dynamics Experiment Simulations: Shrinks with observing time 2.2 nights/month over 15 years will deliver any one of these sets of Grows with time points. Different sets correspond to different target � t = 15 years selection strategies.

  32. Cosmic Dynamics Experiment • 1.7 nights/month over 20 years will unequivocally prove the existence of dark energy without assuming flatness, using any other cosmological constraints or making any � t = 20 years other astrophysical assumption whatsoever. • Provides independent confirmation of SNIa results, using a different method and complementary redshift range. • Data will enable lots of other science (e.g. varying � ), enormous legacy value.

  33. Age of Universe 14.2 ± 2.5 Gyr UVES Cayrel et al. 2001

  34. Part 2: Evolution of the components of the Universe • History of the mass assembly of galaxies: multiwavelength surveys, 3D studies of galaxies • Ly � forest as probe of distant galaxies and IGM • GRBs: galaxies and IGM far and near

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend