Large-angle anomalies in the microwave background: Are they real? What do they mean? Ted Bunn University of Richmond TexPoint fonts used in EMF. Read the.

Slides:



Advertisements
Similar presentations
Primordial perturbations and precision cosmology from the Cosmic Microwave Background Antony Lewis CITA, University of Toronto
Advertisements

CMB and cluster lensing Antony Lewis Institute of Astronomy, Cambridge Lewis & Challinor, Phys. Rept : astro-ph/
If the universe were perfectly uniform, then how come the microwave background isn’t uniform? Where did all the structure(galaxies, clusters, etc.) come.
Foreground cleaning in CMB experiments Carlo Baccigalupi, SISSA, Trieste.
Cleaned Three-Year WMAP CMB Map: Magnitude of the Quadrupole and Alignment of Large Scale Modes Chan-Gyung Park, Changbom Park (KIAS), J. Richard Gott.
Systematic effects in cosmic microwave background polarization and power spectrum estimation SKA 2010 Postgraduate Bursary Conference, Stellenbosch Institute.
Dark Energy Observations of distant supernovae and fluctuations in the cosmic microwave background indicate that the expansion of the universe is accelerating.
30/8/2005COSMO-05, Bonn CMB and the Topology of the Universe Dmitri Pogosyan, UAlberta With: Tarun Souradeep Dick Bond and: Carlo Contaldi Adam Hincks.
Is the Universe homogeneous and isotropic? Marc Kamionkowski (Caltech) Tsvi-fest, 17 December 2009 Statistically.
Dark Energy Cosmology INPE Winter School September 12-16, 2005 Robert Caldwell Dartmouth College.
Component Separation of Polarized Data Application to PLANCK Jonathan Aumont J-F. Macías-Pérez, M. Tristram, D. Santos
The Cosmic Microwave Background. Maxima DASI WMAP.
Measuring the local Universe with peculiar velocities of Type Ia Supernovae MPI, August 2006 Troels Haugbølle Institute for Physics.
The Curvature Perturbation from Vector Fields: the Vector Curvaton Case Mindaugas Karčiauskas Dimopoulos, Karčiauskas, Lyth, Rodriguez, JCAP 13 (2009)
Higher Order Multipole Transition Effects in the Coulomb Dissociation Reactions of Halo Nuclei Dr. Rajesh Kharab Department of Physics, Kurukshetra University,
Patricio Vielva Astrophysics Department (IFCA, Santander) Currently Astrophysics Group (Cavendish Lab., Cambridge) Wiaux, Vielva, Martínez-González.
University of Århus lunch talk, May 11, 2007 Large angle CMB anomalies and local structures Syksy Räsänen CERN Syksy Räsänen CERN.
Introduction to Power Spectrum Estimation Lloyd Knox (UC Davis) CCAPP, 23 June 2010.
What have we learnt from WMAP? Robert Crittenden Institute of Cosmology and Gravitation, Portsmouth, UK.
Evidence for Large Scale Anisotropy in the Universe Pankaj Jain I.I.T. Kanpur.
Nidhi Joshi Centre for Theoretical Physics Jamia Millia Islamia Collaborators: Aditya Rotti, Tarun Souradeep Confronting particle-cosmology with Planck.
Is there a preferred direction in the Universe P. Jain, IIT Kanpur There appear to be several indications of the existence of a preferred direction in.
Objectives of Multiple Regression
Glenn Starkman Dept. of Physics/CERCA/ISO Case Western Reserve University June 10-12, 2015 Princeton, NJ IAS Princeton, NJ Collaborators: C. Copi,
Cosmic Microwave Background (CMB) Peter Holrick and Roman Werpachowski.
Cosmology, University of Bologna – May Cosmology: Polarization of the Cosmic Microwave Background Steven T. Myers University of Bologna and the.
Weak Lensing 3 Tom Kitching. Introduction Scope of the lecture Power Spectra of weak lensing Statistics.
Evidence Based Medicine
Example 10.1 Experimenting with a New Pizza Style at the Pepperoni Pizza Restaurant Concepts in Hypothesis Testing.
THE LARGE SCALE CMB CUT-OFF AND THE TENSOR-TO-SCALAR RATIO Gavin Nicholson Imperial College London with Carlo Contaldi Imperial College London (astro-ph/ )
L. Perivolaropoulos Department of Physics University of Ioannina Open page.
Relic Anisotropy as the source of all Evil? Carlo Contaldi Imperial College London + Marco Peloso & Emir Gumrukcuoglu University of Minnesota, Minneapolis.
ArXiv: [hep-ph] arXiv: [astro-ph.CO] With Konstantinos Dimopoulos and Mindaugas Karčiauskas. Jacques M. Wagstaff VECTOR CURVATON MODEL.
CMB observations and results Dmitry Pogosyan University of Alberta Lake Louise, February, 2003 Lecture 1: What can Cosmic Microwave Background tell us.
Probing fundamental physics with CMB B-modes Cora Dvorkin IAS Harvard (Hubble fellow) Status and Future of Inflationary Theory workshop August 2014, KICP.
Research Process Parts of the research study Parts of the research study Aim: purpose of the study Aim: purpose of the study Target population: group whose.
CMB Polarization from Patchy Reionization Gil Holder.
PHY306 1 Modern cosmology 4: The cosmic microwave background Expectations Experiments: from COBE to Planck  COBE  ground-based experiments  WMAP  Planck.
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.
Anomalies of low multipoles of WMAP
Hemispherical Power Asymmetry 郭宗宽 昆明 anomalies in CMB map the quadrupole-octopole alignment power deficit at low- l hemispherical asymmetry.
Cosmic Microwave Background Carlo Baccigalupi, SISSA CMB lectures at TRR33, see the complete program at darkuniverse.uni-hd.de/view/Main/WinterSchoolLecture5.
February 16, 2009Scott Dodelson, AAAS Meeting Gravitational Waves as a Probe of the Early Universe.
Collaborators within DK-Planck community Lung-Yih Chiang (NBI) Andrei Doroshkevich (TAC,ASC FIRAN) Per Rex Christensen (NBI) Igor D. Novikov ( NBI) Pavel.
BBN: Constraints from CMB experiments Joanna Dunkley University of Oxford IAUS Geneva, Nov
The Planck Satellite Hannu Kurki-Suonio University of Helsinki Finnish-Japanese Workshop on Particle Cosmology, Helsinki
Correlation. Correlation Analysis Correlations tell us to the degree that two variables are similar or associated with each other. It is a measure of.
The Beginning of Time: Evidence for the Big Bang & the Theory of Inflation.
Adventures in Parameter Estimation Jason Dick University of California, Davis.
6dF Workshop April Sydney Cosmological Parameters from 6dF and 2MRS Anaïs Rassat (University College London) 6dF workshop, AAO/Sydney,
Bwdem – 06/04/2005doing cosmology with galaxy clusters Cosmology with galaxy clusters: testing the evolution of dark energy Raul Abramo – Instituto de.
Quantum Noises and the Large Scale Structure Wo-Lung Lee Physics Department, National Taiwan Normal University Physics Department, National Taiwan Normal.
Remote Quadrupole Measurements from Reionization Gil Holder Collaborators: Jon Dudley; Alex van Engelen (McGill) Ilian Iliev (CITA/Zurich); Olivier Dore.
CMB, lensing, and non-Gaussianities
Feasibility of detecting dark energy using bispectrum Yipeng Jing Shanghai Astronomical Observatory Hong Guo and YPJ, in preparation.
Large Scale Anisotropy in the Universe Pankaj Jain I.I.T. Kanpur.
G. Cowan Lectures on Statistical Data Analysis Lecture 10 page 1 Statistical Data Analysis: Lecture 10 1Probability, Bayes’ theorem 2Random variables and.
Szapudi´s talk – False Detection Rate Simultaneous hypothesis testing - Setting the statistical significance Detections of Non-Gaussianity in CMB observations.
Tests of Significance We use test to determine whether a “prediction” is “true” or “false”. More precisely, a test of significance gets at the question.
BICEP2 Results & Its Implication on inflation models and Cosmology Seokcheon Lee 48 th Workshop on Gravitation & NR May. 16 th
Step 1: Specify a null hypothesis
Large Scale Anisotropy in the Universe
Testing Primordial non-Gaussianities in CMB Anisotropies
Cosmological constraints from μE cross correlations
Bayesian Estimation of the isotropy violation in the CMB sky
Shintaro Nakamura (Tokyo University of Science)
Inflation and the cosmological density perturbation
Chapter 12 Power Analysis.
The Axis of Evil: revisited
CMB Anisotropy 이준호 류주영 박시헌.
Presentation transcript:

Large-angle anomalies in the microwave background: Are they real? What do they mean? Ted Bunn University of Richmond TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AA A A AA A A

CMB anisotropy is incredibly consistent with the standard model… but some claims have been made of unexpected features on large angular scales. Anomalies may not mean anything! (a posteriori statistics) March 16, 2010Moriond

Puzzles I’ll focus on Large-scale power deficit North-south asymmetry Alignment of multipoles (“axis of evil”) March 16, 2010Moriond

Is there anything to explain? How not to do statistics: 1.Notice something strange in your data. 2.Devise a statistic a posteriori to quantify how strange it is. 3.Take seriously the p -values derived from that statistic. All claimed anomalies suffer from this problem to some extent  Argument for ignoring the whole subject. But… We use “invalid” statistical methods all the time, relying on intuition and further tests to keep us honest. If these anomalies are real, they’re important! My unjustified opinion: We should proceed, but with skepticism. March 16, 2010Moriond

Example A simulated CMB map, made in the “usual” way (Gaussian, statistically isotropic) and smoothed to show only large-scale features: The two most extreme hot spots are almost perfectly antipodal and cause positive skewness. Easy to devise statistics to show this is unlikely at > 99% confidence. March 16, 2010Moriond

Should we care about the large-angle anomalies? My (unjustified) opinions: The problem of a posteriori statistics is a reason to tread carefully, but not a reason to dismiss the whole subject outright. » We use “invalid” statistical methods all the time in science, and rely on our intuition to decide whether it’s OK. The possibility that the CMB is telling us something nonstandard about the largest-scale features in the Universe is very exciting – worth looking into. March 16, 2010Moriond

Anomaly 1: Lack of large-scale power Low quadrupole C 2 » Large cosmic variance + need to mask  statistical significance is not strong. Discrepancy looks much more striking when phrased in terms of the real- space correlation function, instead of the spherical harmonic coefficients. is low compared to standard model at 99.8% confidence (Copi et al. 2006). March 16, 2010Moriond

How a posteriori is this? Specific statistic S 1/2 : Very. Looking at the correlation function instead of the power spectrum: Not at all. » C(  ) was the standard tool in the old days, especially on small scales. My opinion: The fact that C(  ) is essentially zero for large angles is intriguing. March 16, 2010Moriond Smoot et al Alsop et al. 1991

What could it mean? Possibilities: 1.Statistical fluke 2.Foreground 3.Systematic error 4.New physics (topology, …) Theorem: No independent additive contaminant to the standard model can explain this anomaly: March 16, 2010Moriond P(with contaminant) < P(without contaminant) (Copi et al. 06, Bunn & Bourdon 08) If a contaminant is invoked to explain any other problem, it worsens this one!

Anomaly 2: Hemisphere asymmetry ~10% more fluctuation power in one hemisphere than in the other. Initial tests: p ~.01. March 16, 2010Moriond Eriksen et al 2003 Ratio of hemisphere power spectra, l=2-63.

Why you should take this seriously Tests done for multiple different ranges of l. Directions of asymmetry are similar. If standard model is right, these should be independent random directions. All but the first one can be thought of as a priori. March 16, 2010Moriond Hansen et al 2008

Anomaly 3: Alignment of multipoles  Maps with l=2,3 pick out approximately the same plane on the sky.  l=3 map is more planar than expected.  Normal to plane lies near ecliptic, CMB dipole. Depending on which of these “surprises” you include, formal statistical significance can be p ~ My unjustified opinion: This is the sort of pattern that humans are good at spotting, whether or not it’s there. March 16, 2010Moriond Hinshaw et al. 2007

Possible explanations? Each anomaly could be due to a fluke, systematic error, foreground, or new physics. Sample possibilities for new physics: » Spontaneous isotropy breaking (Gordon et al.) : Radiation field couples to some other field, with only large-scale fluctuations. » Preferred direction picked out during inflation (Ackerman et al.). March 16, 2010Moriond

Do the data justify a more complicated model? Bayesian evidence: One way of deciding whether to prefer a more complicated theory: » Evidence ratio = Factor by which posterior probability ratio changes as a result of the data. » Complicated theories automatically disfavored. In all cases examined so far, BE provides only weak to moderate support for the nonstandard model. March 16, 2010Moriond Hoftuft et al Zheng & Bunn, in prep. Cutoff in prior Evidence raito SIB1 SIB2 PD Zheng & EB, in prep.

So what should we do? Hard to know how seriously to take any of this! Solution to the problem of a posteriori statistics: Get a new data set, for which the tests are a priori. Need a data set that probes other perturbation modes on ultralarge scales: » CMB polarization » Large-scale structure / 21 cm tomography? » Kamionkowski-Loeb remote quadrupole measurements? March 16, 2010Moriond

Large-scale power deficit in CMB polarization Define a statistic precisely analogous to S 1/2 for polarization maps. is (nearly) uncorrelated with.  it can be regarded as an a priori statistic. If is anomalously small, then something interesting is happening. February 18, 2010Wisconsin16 All pol

March 16, 2010Moriond Remote quadrupole measurements CMB photons scatter in a galaxy cluster. Induced polarization tells us the CMB quadrupole at the cluster’s location & look-back time. Strength of signal < 1  K. Hard but not impossible. Lets us measure new modes of the radiation field on the scales corresponding to l ~ Our LSS Us Galaxy Cluster (Kamionkowski & Loeb 1997; Bunn 2006) Cluster LSS

Conclusions Large-angle CMB anomalies don’t “prove” that anything nonstandard is going on, but may provide hints of places to look for interesting phenomena on large scales. Important to make predictions and choose statistics in advance for new data sets, to avoid a posteriori statistics. March 16, 2010Moriond