SENSITIVITY OF COSMOLOGICAL DATA TO THE NEUTRINO MASS HIERARCHY

Similar documents
THE HUNT FOR NEUTRINO HIERARCHY

NEUTRINO PROPERTIES FROM COSMOLOGY

Planck constraints on neutrinos. Massimiliano Lattanzi Università di Ferrara on behalf of the Planck Collaboration

Probing Neutrino Properties with Astrophysics: Neutrino Masses

Neutrinos in the era of precision Cosmology

Cosmological Constraints from the XMM Cluster Survey (XCS) Martin Sahlén, for the XMM Cluster Survey Collaboration The Oskar Klein Centre for

Finding an Upper Bound on Neutrinos Mass

Finding Neutrinos Mass Upper Bound

Status of neutrino mass-mixing parameters and implications for single and double beta decay searches

Absolute Neutrino Mass from Cosmology. Manoj Kaplinghat UC Davis

Kinetic Sunyaev-Zel dovich effect: Dark Energy, Modified gravity, Massive Neutrinos

NEUTRINO COSMOLOGY. n m. n e. n t STEEN HANNESTAD UNIVERSITY OF AARHUS PLANCK 06, 31 MAY 2006

PLANCK lately and beyond

Large Scale Structure After these lectures, you should be able to: Describe the matter power spectrum Explain how and why the peak position depends on

Measuring Neutrino Masses and Dark Energy

Neutrinos secretly converting to lighter particles to please both KATRIN and Cosmos. Yasaman Farzan IPM, Tehran

Future precision cosmology and neutrinos

CMB Constraints on Fundamental Physics

Introduction to CosmoMC

Neutrinoless Double Beta Decay for Particle Physicists

Cosmological constraints on the Sessaw Scale

The ultimate measurement of the CMB temperature anisotropy field UNVEILING THE CMB SKY

The Nature and Magnitude of Neutrino Mass

CosmoSIS Webinar Part 1

arxiv: v2 [astro-ph.co] 14 Nov 2017

K. Zuber, TU Dresden INT, Double beta decay experiments

Planck 2015 parameter constraints

Searching for neutrino- less double beta decay with EXO- 200 and nexo

Possible sources of very energetic neutrinos. Active Galactic Nuclei

Recent T2K results on CP violation in the lepton sector

To Be or Not To Be: Majorana Neutrinos, Grand Unification, and the Existence of the Universe

Combining and comparing neutrinoless double beta decay experiments using. using different nuclei

Steen Hannestad Department of Physics and Astronomy, Aarhus University, Ny Munkegade, DK-8000 Aarhus C, Denmark

Neutrino Mass: Overview of ββ 0ν, Cosmology and Direct Measurements Carlo Giunti

Cosmology after Planck

CMB & Light Degrees of Freedom

Cosmology with CMB & LSS:

Constraints on primordial abundances and neutron life-time from CMB

What I heard about Planck Eiichiro Komatsu (MPA) December 9, 2014 December 22, 2014

Recent results from Super-Kamiokande

Reines and Cowan Experiement

Neutrinos in Cosmology (IV)

Thermal Axion Cosmology

Highlights from Planck 2013 cosmological results Paolo Natoli Università di Ferrara and ASI/ASDC DSU2013, Sissa, 17 October 2013

The CMB and Neutrinos

NEUTRINO COSMOLOGY. ν e ν µ. ν τ STEEN HANNESTAD UNIVERSITY OF AARHUS PARIS, 27 OCTOBER 2006

Constraints on Neutrino Physics from Cosmology

German physicist stops Universe

Concordance Cosmology and Particle Physics. Richard Easther (Yale University)

Cosmic Inflation and Neutrino Masses at POLARBEAR CMB Polarization Experiment

Dark Matter Halos in Warm Dark Matter Models

Neutrino properties from cosmology

DARK MATTER. Martti Raidal NICPB & University of Helsinki Tvärminne summer school 1

Introduction to COSMOMC

The first light in the universe

Updating the Status of Neutrino Physics

Implications of cosmological observables for particle physics: an overview

Data analysis of massive data sets a Planck example

Large Scale Bayesian Inference

Overview of Reactor Neutrino

Cosmological Constraints from a Combined Analysis of Clustering & Galaxy-Galaxy Lensing in the SDSS. Frank van den Bosch.

Observational Cosmology

Cosmology with Planck clusters. Nabila Aghanim IAS, Orsay (France)

Mass hierarchy determination in reactor antineutrino experiments at intermediate distances. Promises and challenges. Petr Vogel, Caltech

Dark Matter -- Astrophysical Evidences and Terrestrial Searches

BAO & RSD. Nikhil Padmanabhan Essential Cosmology for the Next Generation VII December 2017

The impact of relativistic effects on cosmological parameter estimation

Neutrino Physics II. Neutrino Phenomenology. Arcadi Santamaria. TAE 2014, Benasque, September 19, IFIC/Univ. València

Two hot issues in neutrino physics

The State of Tension Between the CMB and LSS

Neutrinos and Cosmos. Hitoshi Murayama (Berkeley) Texas Conference at Stanford Dec 17, 2004

Scale symmetry a link from quantum gravity to cosmology

Measuring the neutrino mass hierarchy with atmospheric neutrinos in IceCube(-Gen2)

PoS(CKM2016)117. Recent inclusive tt cross section measurements. Aruna Kumar Nayak

UHE NEUTRINOS AND THE GLASHOW RESONANCE

The T2K experiment Results and Perspectives. PPC2017 Corpus Christi Mai 2017 Michel Gonin On behalf of the T2K collaboration

CMB constraints on dark matter annihilation

Single versus multi field inflation post Planck Christian Byrnes University of Sussex, Brighton, UK. Kosmologietag, Bielefeld.

The Dark Matter Problem

Effective Field Theory approach for Dark Energy/ Modified Gravity. Bin HU BNU

A profile likelihood analysis of the CMSSM with Genetic Algorithms

Determining neutrino masses from cosmology

Active Learning for Fitting Simulation Models to Observational Data

The Hunt for Sterile Neutrinos. H. Ray, University of Florida

LOW ENERGY SOLAR NEUTRINOS WITH BOREXINO. Lea Di Noto on behalf of the Borexino collaboration

Final status of L3 Standard Model Higgs searches and latest results from LEP wide combinations. Andre Holzner ETHZ / L3

H 0 is Undervalued BAO CMB. Wayne Hu STSCI, April 2014 BICEP2? Maser Lensing Cepheids. SNIa TRGB SBF. dark energy. curvature. neutrinos. inflation?

Recent Results from T2K and Future Prospects

New Results for ν µ ν e oscillations in MINOS

PoS(NOW2016)003. T2K oscillation results. Lorenzo Magaletti. INFN Sezione di Bari

Cosmological neutrinos

Cosmology with Planck: Nucleosynthesis and neutron life-time constraints

Down-to-earth searches for cosmological dark matter

PROBING THE MASS HIERARCHY WITH SUPERNOVA NEUTRINOS

Sensitivity of CP Majorana phases using the synergy between cosmological and neutrinoless double beta decay data at high precision era of measures

Exploring the Lifetime Frontier and Cosmic Ray Physics

Is nonstandard interaction a solution to the three neutrino tensions?

MINOS Result. The ND analysis predicts: events in the Far Detector 54 observed, 0.7σ excess. 49.1±7.0(stat.)±2.7(syst.

Detection of Pre-supernova neutrinos

Neutrino Mass Hierarchy and other physics in H 2 0 (ORCA & PINGU) Aart Heijboer Nikhef, Amsterdam, KM3NeT collaboration

Transcription:

SENSITIVITY OF COSMOLOGICAL DATA TO THE NEUTRINO MASS HIERARCHY Martina Gerbino Oskar Klein Centre for Cosmoparticle Physics Stockholm University TeVPA 2017, Columbus - OH 9 Aug 2017 based on Gerbino,Lattanzi,Mena,Freese,2017

What we know, from the outside How do they behave? Neutrinos oscillate, so they are massive 0.06 ev < m < 6 ev Count rate m =0 m =1.0 ev Lower bound from oscillation experiments Energy (kev) Upper bound from kinematic measurements

Massive neutrinos alter background and perturbation evolution Linear regime ends roughly here { 3 H{+1L C { ê2p @10 9 mk 2 D 1.8 1.6 1.4 1.2 1.0 0.8 Sm n = 0.06 ev Sm n = 0.2 ev Sm n = 0.4 ev Sm n = 0.6 ev Sm n = 0.8 ev 0.6 0.4 500 1000 1500 2000 2500 WMAP9 data end here { credits: M.Lattanzi Abazaijan+,2015 3 active families, sub-ev masses Relativistic at early times, non-relativistic today (Almost) peculiar effects on cosmological observables See M. Lattanzi & A. van Engelen s talks

Joint constraints on Mnu - future CMB-S4 Science Book ~3sigma detection in the minimal mass scenario with S4 surveys

Will we be able to discriminate the hierarchy? Can we provide a statistically robust answer?

The proposed method Bayesian MCMC, Mnu + other cosmo params + h Discrete Hyper-parameter h h=nh h=ih NORMAL HIERARCHY m,1 = m light q m,2 = m 2 1 + m2 12 q m,3 = m 2 1 + m2 13 Advantages: INVERTED HIERARCHY m,3 = m light q m,1 = m 2 3 + m2 13 q m,2 = m 2 1 + m2 12 neutrinos modelled with exact mass spectrum information from oscillations taken into account quantifies sensitivity to the hierarchy takes into account uncertainties related to the hierarchy Gerbino,Lattanzi,Mena,Freese 2017

Sensitivity to the hierarchy P/Pmax 1.0 0.8 0.6 0.4 0.2 0.0 TT+lowP TT+lowP+BAO TT,TE,EE+lowP TT,TE,EE+lowP+BAO CURRENT LIMITS 0.25 0.50 0.75 1.00 M [ev] P/Pmax 1.0 0.8 0.6 0.4 0.2 0.0 COrE,M fid = 0.06 ev COrE+BAO,M fid COrE,M fid = 0.1 ev COrE+BA=,M fid = 0.06 ev = 0.1 ev FORECASTS 0.10 0.15 0.20 0.25 M [ev] Gerbino,Lattanzi,Mena,Freese 2017 P(h = NH):P(h = IH) 3:2 See also Hannestad&Schwetz 2016, Couchot et al 2017, Capozzi et al 2017 P(h = NH):P(h = IH) 0.06eV mass -> 9:1 0.1eV mass -> 1:1 Martina Gerbino, TeVPA - Cosmology track, 9Aug2017

Sensitivity to the hierarchy Fixed fiducial As sigma increases, NH is as likely as IH Fixed sigma NH favoured for Mnu<0.1eV, IH favoured for Mnu~0.1eV, no preference for Mnu>0.1eV

CONCLUSIONS Tight bounds on neutrino mass from cosmology Inverted hierarchy in trouble: how much? By introducing an hyper-parameter we can: 1) easily account for exact neutrino mass spectra; 2) quantify sensitivity to the hierarchy; 3) take into account uncertainty due to imperfect knowledge of the hierarchy NH favoured 5:3 by current data NH favoured 10:1 by future measurements, if the mass is minimal sensitivity driven by prior choice

BACK-UP Martina Gerbino, TeVPA - Cosmology track, 9Aug2017

The standard method M nu (+other cosmological parameters) Degenerate spectrum: m,i = M /3, i=1, 2, 3 0.1eV Different authors obtain upper bounds from current data approaching the critical value of 0.1 ev. These results suggest that IH starts to get under pressure from cosmology. [ ] Such a claim should be based on a proper statistical analysis. The question to be answered is, whether the hypothesis of IH can be rejected with some confidence against NH. (Hannestad&Schwetz,2016)

Joint constraints on Mnu - present Vagnozzi,Giusarma,Mena,Freese,MG,Ho,Lattanzi 2017 M i m,i Planck TT+lowP+BAO: Mnu<0.2eV Planck TT+lowP+Pk: Mnu<0.3eV Planck TT+lowP+BAO+Pk: Mnu<0.25eV Compilation of CMB and LSS data 95% CL major improvement with a better measurement of the optical depth and/or use of CMB small scale polarisation: wait for Planck legacy release! Take home message: tight, yet robust bounds

Sensitivity to the hierarchy Physical effects due to different distribution of the sum of the masses for the 2 hierarchies Total nu energy density Matter power spectrum Lesgourgues&Pastor, 2006 Are current (and future) data sensitive to these effects? How much?

Sensitivity to the hierarchy m bb @evd 0.003 0.01 0.03 0.1 KamLAND-Zen H90% upper boundl M fid = 0.06 ev 0.03 0.1 M n @evd nexo 10yr wê Ba tag H90% upper boundl m bb @evd 0.003 0.01 0.03 0.1 KamLAND-Zen H90% upper boundl M fid =0.1 ev 0.03 0.1 M n @evd If Mnu=0.1eV, sigma(mbb)~10mev could guarantee 0n2b measurement nexo 10yr wê Ba tag H90% upper boundl 0n2b could in turn helps unravel the hierarchy (wip, extending the results in Gerbino+2015 in the hierarchical bayesian context) Gerbino,Lattanzi,Mena,Freese 2017