Title people CHIME: the Canadian Hydrogen Intensity Mapping Experiment. Mark Halpern Kris Sigurdson Sigi Stiemer Tom Landecker Jeff Peterson Dick Bond.

Slides:



Advertisements
Similar presentations
Seeing Dark Energy (or the cosmological constant which is the simplest form of DE) Professor Bob Nichol (ICG, Portsmouth)
Advertisements

21cm cosmology T. Chang, UP, J. Peterson, P. McDonald PRL 100, (2008) UP, L. Staveley-Smith, J. Peterson, T. Chang, MNRAS, 394, 6 (2009)
21 cm Cosmology Jeff Peterson, CMU -Existing telescopes and data -Intensity Mapping -Fixed Cylinders.
Cosmology using 21 cm emission Jeff Peterson, CMU Talk 1…Update on early ionization telescopes (LOFAR, PAST, GMRT) Talk 2…Proposed Redshift survey.
Dark Energy BAO Intensity Mapping T. Chang, UP, J. Peterson, P. McDonald PRL 100, (March 5, 2008) UP, L. Staveley-Smith, J. Peterson, T. Chang arXiv:
Weighing Neutrinos including the Largest Photometric Galaxy Survey: MegaZ DR7 Moriond 2010Shaun Thomas: UCL “A combined constraint on the Neutrinos” Arxiv:
Planck 2013 results, implications for cosmology
Astronomy and the Electromagnetic Spectrum
Hydrogen 21cm Cosmology Tzu-Ching Chang (ASIAA)
What Figure of Merit Should We Use to Evaluate Dark Energy Projects? Yun Wang Yun Wang STScI Dark Energy Symposium STScI Dark Energy Symposium May 6, 2008.
CMB: Sound Waves in the Early Universe Before recombination: Universe is ionized. Photons provide enormous pressure and restoring force. Photon-baryon.
Observational Cosmology - a laboratory for fundamental physics MPI-K, Heidelberg Marek Kowalski.
Cosmological Information Ue-Li Pen Tingting Lu Olivier Dore.
Observational Cosmology - a unique laboratory for fundamental physics Marek Kowalski Physikalisches Institut Universität Bonn.
The National Science Foundation The Dark Energy Survey J. Frieman, M. Becker, J. Carlstrom, M. Gladders, W. Hu, R. Kessler, B. Koester, A. Kravtsov, for.
Lecture 2: Observational constraints on dark energy Shinji Tsujikawa (Tokyo University of Science)
Nikolaos Nikoloudakis Friday lunch talk 12/6/09 Supported by a Marie Curie Early Stage Training Fellowship.
Universe in a box: simulating formation of cosmic structures Andrey Kravtsov Department of Astronomy & Astrophysics Center for Cosmological Physics (CfCP)
PRE-SUSY Karlsruhe July 2007 Rocky Kolb The University of Chicago Cosmology 101 Rocky I : The Universe Observed Rocky II :Dark Matter Rocky III :Dark Energy.
July 7, 2008SLAC Annual Program ReviewPage 1 Future Dark Energy Surveys R. Wechsler Assistant Professor KIPAC.
Neutrinos in Cosmology Alessandro Melchiorri Universita’ di Roma, “La Sapienza” INFN, Roma-1 NOW-2004, 16th September, 2004.
Signe Riemer-Sørensen, University of Queensland In collaboration with C. Blake (Swinburne), D. Parkinson (UQ), T. Davis (UQ) and the WiggleZ collaboration.
Dark Energy and Cosmic Sound Daniel Eisenstein (University of Arizona) Michael Blanton, David Hogg, Bob Nichol, Nikhil Padmanabhan, Will Percival, David.
Cosmic Microwave Background (CMB) Peter Holrick and Roman Werpachowski.
P olarized R adiation I maging and S pectroscopy M ission Probing cosmic structures and radiation with the ultimate polarimetric spectro-imaging of the.
PHY306 1 Modern cosmology 4: The cosmic microwave background Expectations Experiments: from COBE to Planck  COBE  ground-based experiments  WMAP  Planck.
The Science Case for the Dark Energy Survey James Annis For the DES Collaboration.
Polarization-assisted WMAP-NVSS Cross Correlation Collaborators: K-W Ng(IoP, AS) Ue-Li Pen (CITA) Guo Chin Liu (ASIAA)
Early times CMB.
130 cMpc ~ 1 o z~ = 7.3 Lidz et al ‘Inverse’ views of evolution of large scale structure during reionization Neutral intergalactic medium via HI.
Title people CHIME: the Canadian Hydrogen Intensity Mapping Experiment. Mark Halpern Kris Sigurdson Sigi Stiemer Tom Landecker Jeff Peterson Dick Bond.
Dark energy I : Observational constraints Shinji Tsujikawa (Tokyo University of Science)
Sanjay K. Pandey L.B.S.P.G.College, Gonda (India). Statistical Analysis of Redshifted Neutral Hydrogen.
How can CMB help constraining dark energy? Licia Verde ICREA & Institute of space Sciences (ICE CSIC-IEEC)
Clustering in the Sloan Digital Sky Survey Bob Nichol (ICG, Portsmouth) Many SDSS Colleagues.
Dark Energy Probes with DES (focus on cosmology) Seokcheon Lee (KIAS) Feb Section : Survey Science III.
Lecture 5: Matter Dominated Universe: CMB Anisotropies and Large Scale Structure Today, matter is assembled into structures: filaments, clusters, galaxies,
PHY306 1 Modern cosmology 4: The cosmic microwave background Expectations Experiments: from COBE to Planck  COBE  ground-based experiments  WMAP  Planck.
Yun Wang, 3/2011 Baryon Acoustic Oscillations and DE Figure of Merit Yun Wang Yun Wang WFIRST SDT #2, March 2011 WFIRST SDT #2, March 2011 BAO as a robust.
SUNYAEV-ZELDOVICH EFFECT. OUTLINE  What is SZE  What Can we learn from SZE  SZE Cluster Surveys  Experimental Issues  SZ Surveys are coming: What.
Anadian ydrogen ntensity apping xperiment CHIMECHIME CHIMECHIME WiggleZ Dark Ages Stars 13.7Gy CMB Big Bang Reionization 1100 z∞ SDSS 7Gy CHIME.
PHY306 1 Modern cosmology 3: The Growth of Structure Growth of structure in an expanding universe The Jeans length Dark matter Large scale structure simulations.
Mário Santos1 EoR / 21cm simulations 4 th SKADS Workshop, Lisbon, 2-3 October 2008 Epoch of Reionization / 21cm simulations Mário Santos CENTRA - IST.
BAOs SDSS, DES, WFMOS teams (Bob Nichol, ICG Portsmouth)
The Planck Satellite Hannu Kurki-Suonio University of Helsinki Finnish-Japanese Workshop on Particle Cosmology, Helsinki
Bwdem – 06/04/2005doing cosmology with galaxy clusters Cosmology with galaxy clusters: testing the evolution of dark energy Raul Abramo – Instituto de.
Latest Results from LSS & BAO Observations Will Percival University of Portsmouth StSci Spring Symposium: A Decade of Dark Energy, May 7 th 2008.
THE CONNECTION OF NEUTRINO PHYSICS WITH COSMOLOGY AND ASTROPHYSICS STEEN HANNESTAD CERN, 1 OCTOBER 2009 e    
Complementary Probes of Dark Energy Josh Frieman Snowmass 2001.
1 Baryon Acoustic Oscillations Prospects of Measuring Dark Energy Equation of State with LAMOST Xuelei Chen ( 陳學雷 ) National Astronomical Observatory of.
Dark Energy and baryon oscillations Domenico Sapone Université de Genève, Département de Physique théorique In collaboration with: Luca Amendola (INAF,
The Planck Satellite Matthew Trimble 10/1/12. Useful Physics Observing at a redshift = looking at light from a very distant object that was emitted a.
Brenna Flaugher for the DES Collaboration; DPF Meeting August 27, 2004 Riverside,CA Fermilab, U Illinois, U Chicago, LBNL, CTIO/NOAO 1 Dark Energy and.
Probing Dark Energy with Cosmological Observations Fan, Zuhui ( 范祖辉 ) Dept. of Astronomy Peking University.
Baryon Acoustic Oscillations
Carlos Hernández-Monteagudo CE F CA 1 CENTRO DE ESTUDIOS DE FÍSICA DEL COSMOS DE ARAGÓN (CE F CA) J-PAS 10th Collaboration Meeting March 11th 2015 Cosmology.
Cheng Zhao Supervisor: Charling Tao
Jochen Weller Decrypting the Universe Edinburgh, October, 2007 未来 の 暗 黒 エネルギー 実 験 の 相補性.
Cosmological Structure with the Lyman Alpha Forest. Jordi Miralda Escudé ICREA, Institut de Ciències del Cosmos University of Barcelona, Catalonia Edinburgh,
The Dark Side of the Universe L. Van Waerbeke APSNW may 15 th 2009.
Title 21 cm Intensity Mapping for BAO and CHIME. Temperature - the imprint of BAO is visible in the co-added degree-scale hot (left) & cold (right) spots.
Princeton University & APC
Complementarity of Dark Energy Probes
STRUCTURE FORMATION MATTEO VIEL INAF and INFN Trieste
Cosmology from Large Scale Structure Surveys
A Measurement of CMB Polarization with QUaD
Precision cosmology, status and perspectives
Images: M. Blanton. Images: M. Blanton Figures: M. Blanton & SDSS.
Detection of integrated Sachs-Wolfe effect by cross-correlation of the
6-band Survey: ugrizy 320–1050 nm
Presentation transcript:

title people CHIME: the Canadian Hydrogen Intensity Mapping Experiment. Mark Halpern Kris Sigurdson Sigi Stiemer Tom Landecker Jeff Peterson Dick Bond Ue-Li Pen Matt Dobbs David Hanna UBC DRAO Carnegie Mellon CITA McGill

title people We have proposed to build a new telescope, CHIME, to study Baryon Acoustic Oscillations at the DRAO. The telescope will consist of 5 NS cylindrical reflectors coupled to a large digital correlator and will perform hydrogen intensity mapping of redshifted 21cm radiation. Plan of the talk: 1. What are Baryon Acoustic Oscillations? 2. What will CHIME look like?

Evolution of a density spike in co-moving coordinates. Notice when neutrinos and then photons decouple from baryons. Animation: SDSS Collaboration

Eisenstein et al ApJ

107/h = 148 h= 0.72 Eisenstein et al ApJ

BAO have, of course, been seen in the CMB. They form the “shape” of each hot or cold spot. Komatsu et al Hinshaw et al Komatsu et al. 2010

2.The cosmological constant is only one possibility for the nature of dark energy. In a  dominated universe pressure is negative: P/  w, but in general w can be a function of time or redshift, w(z). To measure how w(z) evolves we need to measure at least one of: A. Angular sizes of a distribution of standard rulers; B. Brightnesses of a distribution of standard candles; or C. Weak lensing patterns. CHIME will supply option A.

DETF Figure of Merit Marginalize over all other parameters and find uncertainties in w  and w a  CDM value w ( a ) = w   w a (  a ) w  w  today & w  w   w a in the far past  DE  DE (today) exp {   [  w (a) ] d ln a }  CDM: w (a)  DETF FoM  1./(area of ellipse) = 450 for the nominal CHIME If built now, CHIME will deliver precision at a tiny cost and well ahead of any competitive experiment.

Figure of Merit for an HI measurement from z 1 to z 2. Given the cell phone wall at 800 MHz, corresponding to z 1 =0.8, there is not much advantage to push the lower freq. Limit beyond z 2 =2.5, or 400 MHz Pushing BAO measurements to low redshift drives the ultimate sensitivity of a survey.

Frequency shift corresp. to  z Redshift d c-m further away. Resolution at z of a 100m telescope The size and frequency resolution of CHIME are chosen to resolve Baryon Acoustic Oscillations in three dimensions. Freq. of redshifted 21cm radiation

CHIME will consist of five 20m x 100m cylindrical reflectors with feeds, amplifiers and digitizers spaced along the 100m focal line.

We have built room temperature amplifiers for CHIME which are much quieter than we had assumed for our sensitivity estimates. This is the work of Greg Davis, UBC.

A CHIME amplifier.

The measured RF Interference at the proposed CHIME site at the DRAO in Penticton looks promising. Measured December 2009 Measurement resolution is 10 kHz. The cell phone band at 850 GHz defines CHIME’s top frequency. Test noise floor is 400K.

CHIME anticipated sensitivity at z=1.5, two years of data. Error bars grow at the right due to finite angular resolution and at the left because CHIME only surveys 40% of the sky Spectrum w. BAO Spectrum w.o. BAO

CHIME will produce data a decade earlier than experiments of comparable sensitivity, and for 1-10% of the cost. Expt. “shot noise” is proportional to survey volume.

1. BLAST resolved the cosmic IR background into emission from 24 um identified galaxies. ‘Canadian’ results from experiments not yet proposed when the last LRP was written:

2. The South Pole Telescope discovered hundreds of new clusters in a blank-field Sunyaev Zeldovich survey. ‘Canadian’ results from experiments not yet proposed when the last LRP was written:

3. The Atacama Cosmology Telescope (ACT) measured the CMB anisotropy at small angular scales. ‘Canadian’ results from experiments not yet proposed when the last LRP was written:

The Canadian Long Range Plan for Astronomy should include support for a plan for funding of important modest-sized experiments with rapid schedules as they arise. The CFI and the CSA have played a sporadic role at this scale and schedule of project, with restrictions. The importance of support for short-notice opportunities to astrophysics in Canada must be made clear.