dark energy and cosmic sound

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Dark Energy and Dark Energy and Cosmic Sound Cosmic Sound Daniel Eisenstein Daniel Eisenstein (University of Arizona) (University of Arizona) Michael Blanton, David Hogg, Bob Michael Blanton, David Hogg, Bob Nichol, Nikhil Padmanabhan, Will Nichol, Nikhil Padmanabhan, Will Percival, David Schlegel, Percival, David Schlegel, Roman Scoccimarro, Ryan Scranton, Hee- Roman Scoccimarro, Ryan Scranton, Hee- Jong Seo, Ed Sirko, David Spergel, Max Jong Seo, Ed Sirko, David Spergel, Max Tegmark, Martin White, Idit Zehavi, Tegmark, Martin White, Idit Zehavi, and the SDSS. and the SDSS.

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Dark Energy and Cosmic Sound. Daniel Eisenstein (University of Arizona) Michael Blanton, David Hogg, Bob Nichol, Nikhil Padmanabhan, Will Percival, David Schlegel, Roman Scoccimarro, Ryan Scranton, Hee-Jong Seo, Ed Sirko, David Spergel, Max Tegmark, Martin White, Idit Zehavi, and the SDSS. - PowerPoint PPT Presentation

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Page 1: Dark Energy and  Cosmic Sound

Dark Energy and Dark Energy and Cosmic SoundCosmic Sound

Daniel EisensteinDaniel Eisenstein(University of Arizona)(University of Arizona)

Michael Blanton, David Hogg, Bob Nichol, Nikhil Michael Blanton, David Hogg, Bob Nichol, Nikhil Padmanabhan, Will Percival, David Schlegel, Padmanabhan, Will Percival, David Schlegel,

Roman Scoccimarro, Ryan Scranton, Hee-Jong Roman Scoccimarro, Ryan Scranton, Hee-Jong Seo, Ed Sirko, David Spergel, Max Tegmark, Seo, Ed Sirko, David Spergel, Max Tegmark,

Martin White, Idit Zehavi, and the SDSS.Martin White, Idit Zehavi, and the SDSS.

Page 2: Dark Energy and  Cosmic Sound

SummarySummary Sound waves that propagate in the first 400,000 years after Sound waves that propagate in the first 400,000 years after

the Big Bang imprint a signature that we can measure in the the Big Bang imprint a signature that we can measure in the clustering of galaxies today: baryon acoustic oscillations.clustering of galaxies today: baryon acoustic oscillations.

This signature has a size that we can calculate accurately. This signature has a size that we can calculate accurately. Measuring this as an angle allows us to infer the distance to Measuring this as an angle allows us to infer the distance to a sample of galaxies.a sample of galaxies.

Measuring accurate distances is a key way to study the Measuring accurate distances is a key way to study the acceleration of the Universe and the properties of dark acceleration of the Universe and the properties of dark energy.energy.

In the last 4 years, astronomers have detected this acoustic In the last 4 years, astronomers have detected this acoustic signature in the clustering of galaxies. Important tool to signature in the clustering of galaxies. Important tool to study cosmological composition.study cosmological composition.

Several new surveys being initiated to push the Several new surveys being initiated to push the measurements to 1% and below.measurements to 1% and below.

Page 3: Dark Energy and  Cosmic Sound

Acoustic Oscillations in the CMBAcoustic Oscillations in the CMB

Although there are fluctuations on all scales, there is a characteristic Although there are fluctuations on all scales, there is a characteristic angular scale. Hot and cold spots tend to be about 1 degree in size.angular scale. Hot and cold spots tend to be about 1 degree in size.

Page 4: Dark Energy and  Cosmic Sound

Acoustic Oscillations in the CMBAcoustic Oscillations in the CMB

WMAP team (Bennett et al. 2003)WMAP team (Bennett et al. 2003)

Acoustic Peaks followa harmonic pattern.

Page 5: Dark Energy and  Cosmic Sound

Sound Waves in the Early UniverseSound Waves in the Early Universe

Before recombination:Before recombination: Universe is ionized. Universe is ionized. Photons provide enormous Photons provide enormous

pressure and restoring force. pressure and restoring force. Perturbations oscillate as Perturbations oscillate as

acoustic waves.acoustic waves.

After recombination:After recombination: Universe is neutral.Universe is neutral. Photons can travel freely Photons can travel freely

past the baryons.past the baryons. Peturbations collapse due Peturbations collapse due

to gravity.to gravity.

Big

Bang Today

Recombinationz ~ 1000

~400,000 yearsIonized Neutral

Time

Page 6: Dark Energy and  Cosmic Sound

Sound WavesSound Waves Each initial overdensity (in DM & gas) Each initial overdensity (in DM & gas)

is an overpressure that launches a is an overpressure that launches a spherical sound wave.spherical sound wave.

This wave travels outwards at This wave travels outwards at 57% of the speed of light.57% of the speed of light.

Pressure-providing photons decouple Pressure-providing photons decouple at recombination. CMB travels to us at recombination. CMB travels to us from these spheres.from these spheres.

Sound speed plummets. Wave stalls Sound speed plummets. Wave stalls at a radius of 150 Mpc.at a radius of 150 Mpc.

Overdensity in shell (gas) and in the Overdensity in shell (gas) and in the original center (DM) both seed the original center (DM) both seed the formation of galaxies. Preferred formation of galaxies. Preferred separation of 150 Mpc.separation of 150 Mpc.

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150 Mpc150 Mpc(500 Mlyr)(500 Mlyr)

Page 7: Dark Energy and  Cosmic Sound

Looking back in time in the Universe

CREDIT: WMAP & SDSS websites

CMB

Looking back in time; angles imply distance

GALA

XIES

Page 8: Dark Energy and  Cosmic Sound

SDSS SDSS Galaxy Galaxy

Redshift Redshift SurveySurvey

200 kpc

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Page 9: Dark Energy and  Cosmic Sound

Correlations of GalaxiesCorrelations of Galaxies

CDM with baryons is a good fit: 2 = 16.1 with 17 dof.Pure CDM rejected at 2 = 11.7

Horizontal match of peak positions allows us to

measure distance to 4%.

Page 10: Dark Energy and  Cosmic Sound

Chasing Sound Across RedshiftChasing Sound Across Redshift

Distance Errors versus RedshiftDistance Errors versus Redshift

Page 11: Dark Energy and  Cosmic Sound

SDSS-IIISDSS-III SDSS-III will be the next phase of the SDSS project, operating SDSS-III will be the next phase of the SDSS project, operating

from summer 2008 to summer 2014.from summer 2008 to summer 2014. SDSS-III has 4 surveys on 3 major themes.SDSS-III has 4 surveys on 3 major themes.

BOSS: Largest yet redshift survey for large-scale structure. Definitive BOSS: Largest yet redshift survey for large-scale structure. Definitive study of the low-redshift acoustic oscillations using study of the low-redshift acoustic oscillations using 1.5 million galaxy redshifts. 1.5 million galaxy redshifts. Goal: 1% measurement of cosmological distance.Goal: 1% measurement of cosmological distance.

SEGUE-2: Optical spectroscopic survey of stars, aimed at structure and SEGUE-2: Optical spectroscopic survey of stars, aimed at structure and nucleosynthetic enrichment of the outer Milky Way.nucleosynthetic enrichment of the outer Milky Way.

APOGEE: Infrared spectroscopic survey of stars, to study the APOGEE: Infrared spectroscopic survey of stars, to study the enrichment and dynamics of the whole Milky Way.enrichment and dynamics of the whole Milky Way.

MARVELS: Multi-object radial velocity planet search.MARVELS: Multi-object radial velocity planet search. Using SDSS telescope, facilities, software.Using SDSS telescope, facilities, software. Strong commitment to public data releases.Strong commitment to public data releases. Collaboration is now forming. Seeking support from Sloan Collaboration is now forming. Seeking support from Sloan

Foundation, DOE, NSF, and over 20 member institutions.Foundation, DOE, NSF, and over 20 member institutions.

Page 12: Dark Energy and  Cosmic Sound

ConclusionsConclusions Acoustic oscillations provide a robust way to Acoustic oscillations provide a robust way to

measure cosmological distance and hence probe measure cosmological distance and hence probe dark energy.dark energy.

SDSS LRG sample uses the acoustic signature to SDSS LRG sample uses the acoustic signature to measure distance to 4% at one redshift.measure distance to 4% at one redshift.

New galaxy surveys in the coming decade will New galaxy surveys in the coming decade will push to 1% and below over a range of redshift.push to 1% and below over a range of redshift.

More information:More information: http://cmb.as.arizona.edu/~eisenste/acousticpeakhttp://cmb.as.arizona.edu/~eisenste/acousticpeak Physics Today article by Daniel Eisenstein & Chuck Physics Today article by Daniel Eisenstein & Chuck

Bennett, April 2008.Bennett, April 2008. http://www.sdss3.org/http://www.sdss3.org/

Page 13: Dark Energy and  Cosmic Sound
Page 14: Dark Energy and  Cosmic Sound

Response of a point perturbationResponse of a point perturbation

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Based on CMBfast outputs (Seljak & Based on CMBfast outputs (Seljak & Zaldarriaga). Green’s function view Zaldarriaga). Green’s function view from Bashinsky & Bertschinger 2001.from Bashinsky & Bertschinger 2001.

Remember: This is a tiny ripple on a big background.