1 / 38

Baryon Acoustic Oscillations Prospects of Measuring Dark Energy Equation of State with LAMOST

1. Baryon Acoustic Oscillations Prospects of Measuring Dark Energy Equation of State with LAMOST. Xuelei Chen ( 陳學雷 ) National Astronomical Observatory of China. KIAS workshop 2008.10.28 Seoul. arxiv:0809.3002. 2. Xin Wang (NAOC) XC Fengquan Wu (NAOC) Zheng Zheng (IAS, Princeton)

lukas
Download Presentation

Baryon Acoustic Oscillations Prospects of Measuring Dark Energy Equation of State with LAMOST

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. 1 Baryon Acoustic OscillationsProspects of Measuring Dark Energy Equation of State with LAMOST Xuelei Chen (陳學雷) National Astronomical Observatory of China KIAS workshop 2008.10.28 Seoul

  2. arxiv:0809.3002 2 Xin Wang (NAOC) XC Fengquan Wu (NAOC) Zheng Zheng (IAS, Princeton) Pengjie Zhang (SHAO) Yongheng Zhao (NAOC)

  3. 3 photon and matter spectrum M. White 2007

  4. 4 Sound Horizon and Peaks in power spectrum model spectrum Peaks at Blake & Glazebrook 2003

  5. 5 Standard Ruler for Cosmology

  6. 6 Combined constraints Percival et al 2007 DV(z=0.35)/DV(0.2)=1.812 +- 0.06

  7. 7 Large Aperture Multi-Optical fiber Spectroscopic Telescope (LAMOST) Located at Xinglong Station (117o 34' E, 40o 23' N)

  8. 8

  9. LAMOST: A meridian reflecting Schmidt telescope • Main features • large aperture (4-meter) • wide field of view (5-degree) • observation only during the meridian transit (1.5-3 hours) of an object • observable sky -10o< dec <+90o ~24000 sqr. deg. • limiting magnitude (1.5hr) b=20.5 • 4000 fibers spectroscopy (3700A-9000A) • spectral resolution R=1000/2000 • total # of spectra (3yr) 107 • Technical innovations • active optics for segmented thin mirrors • parallel controllable fiber positioning

  10. FoV (deg) Diameter (m)

  11. Original Definition of Scientific Goals of LAMOST Wide field & large sample spectroscopy 107 galaxies Large scale structure of Universe, Cosmology Physics of galaxies 107 stars Galactic structure, Stellar physics 106 quasars… Multi-waveband astrophysics

  12. Status and Plan: • Sep 2008, all hardwares in place • going through engineering tests • two workgroups appointed by the Survey Selection • Committee: extragalactic (Yipeng Jing), Milky Way (Licai • Deng); working for overall survey plans • Apr 2009, survey plans • Dec 2008 to 2009/10, commission period • 2010/11-2015, regular spectroscopic survey • data release (2 years after taken)

  13. SDSS MAIN LAMOST MAIN Selecting Targets SDSS photometric catalog as input • generic galaxy survey • LRG survey • quasars SDSS region: about 8000 deg2

  14. 14 Selecting the Targets: Luminous Red Galaxies Luminous Red Galaxies (LRG): bright elliptical galaxies strongly clustered many in clusters or groups easy to determine photometric z

  15. 15 Target Redshift Distribution main1: r<18.8 main2: r<19.8 LAMOST LRG(MegaZ)

  16. 16 To what precision can we measure? Seo & Eisenstein 2003:

  17. 17 Error Estimates

  18. 18 Design the survey: integration time point source (QSO) exponential (spiral galaxy) de Vaucouleurs (elliptical galaxy) assume sky background 20.5 in r and i.

  19. 19 Design the Survey: target surface density Fiber Surface Density: 200 Optimal for fiber positioning: 400-600

  20. Survey ideas 20

  21. 21 Estimate of the Bias of the sample

  22. 22 Estimate Bias Using the HOD model:

  23. 23

  24. LRG bias We assume the HOD parameters given in Brown et al., arxiv:0804.2293 B band vs. other band: we assume matching density b(z=0.475)=1.77, b(z=0.625)=2.29

  25. QSO bias Wyithe & Loeb (2003), Marulli et al (2006) QSO is triggered by major merger

  26. QSO Luminosity Function

  27. QSO bias QSO1: g<20.5, QSO2: g<21.0, QSO3: g<21.65

  28. Comparison with direct observation Porciani et al (2004) use 14000 quasar from 2dF/6dF to measure QSO bias The bias obtained this way is slightly (10%-20%) greater.

  29. 29 Effective Volume

  30. 30 Error on power spectrum

  31. Error on distance scales Caution: error depends on bin size.

  32. 32

  33. 33 Improvement on Dark Energy EoS

  34. 35 Effect of Spectral Resolution on Figure of Merit (inverse of error ellipse area) SDSS: FoM~2

  35. 36 Simulation SDSS LAMOST

  36. 37 Summary • A main survey of 1-2 magnitude deeper than SDSS could improve BAO measurement FoM by a factor of about 3-5. • LRG survey fiber time is much smaller than MAIN1 but could achieve similar effective volume • QSO survey could achieve large effective volume at large scales, but declines rapidly at small scales • For BAO measurement, R=1000 is sufficient and economical • May improve current DE constraint, but still not enough to give accurate answer on varying EoS.

  37. 38 Thanks

More Related