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1 Pijushpani Bhattacharjee 15 Nov 2017 SERC School-EHEP, NISER Dark Matter and its Detection Lectures at SERC School on Experimental High Energy Physics, NISER, Odisa Pijushpani Bhattacharjee Saha Inst. of Nuclear Physics Kolkata Lecture-1: Introduction & Overview

Dark Matter and its Detection - NISERJ. Formaggio and C. Martoff, Ann. Rev. Nucl. Part. Sci. 54 (2004) 361 SERC School-EHEP, NISER Pijushpani Bhattacharjee 15 Nov 2017 48 Exclusion

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  • 1Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Dark Matter and its Detection Lectures at

    SERC School on Experimental High Energy Physics,

    NISER, Odisa

    Pijushpani BhattacharjeeSaha Inst. of Nuclear Physics

    Kolkata

    Lecture-1: Introduction & Overview

  • 2Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Organization of the lectures

    Lecture 1 : Introduction and broad Overview

    Lecture 2/Tutorial : Decoupling and thermal freeze out; calculation of the cosmological relic abundance of weakly interacting massive particles (WIMPs) from the early Universe

    Lecture 3 : Basic phenomenology of direct detection of WIMP candidates of Dark Matter

  • 3Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Some (astronomical) Units

  • 4Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Parsec:

  • 5Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Edwin Hubble and the Expanding Universe

  • 6Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Basic Equations of Cosmology

  • 7Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Hot Big Bang Scenario● The Universe was hotter and denser in the past. Evidence:

    The Cosmic Microwave Background Radiation (CMBR).

    ● At very early times, matter content of the Universe was in

    the form of “fundamental” particles : quarks, & leptons. There were no protons, neutrons, nuclei, and atoms. Those gradually appeared as the Universe expanded and cooled.

    ● Formation of galaxies and other structures, and anisotropies in CMBR, require the presence of some kind of very weakly interacting matter – Dark Matter

  • 8Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

  • 9Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Evidence for Dark Matter(Basic qualitative ideas)

  • 10Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    The “Visible” Universe

    Source: Unknown (Web)

  • 11Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Is what we “see” all that is there in the Universe?

    Evidently, No! (If Newton/Einstein-ian dynamics is valid on all length scales of interest)

    Mass discrepancyTotal gravitating mass in a system estimated from dynamical considerations (for example, from studying the motions of visible objects in the system)

    the total masses of the “visible” matter/objects in the system

  • 12Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    To explain the formation of structures in the expanding Universe that we “see”, we need a lot of additional matter that we don't see! DARK MATTER! – What is it? Is it just normal matter in the form of objects that are too faint to see (e.g., planets, gas, black holes, neutron stars,...) or a completely new kind of fundamental particles?

    – Where is it? Is it only in certain places/objects in the Universe, or is it ubiquitous?

    – How much of it? Uniformly distributed or in clumps?

    – How do we, or can we at all, detect it in some controlled experiments? …. ?

  • 13Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Can't see Dark Matter. Know it's presence only through it's

    Can't directly `see' Dark Matter

    Know its presence only through its gravitational influence on visible matter

  • 14Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Oort (1932) …

    Jan Hendrik Oort (1900-1992)To explain the kinematics of vertical motion of the disk stars, Oort needed “invisible mass” of density ~ 2 GeV / cc at the solar neighborhood.Modern value ~ 0.3 Gev / cc

    We know now that Oort's “invisible” mass mostly consisted of objects too faint to “see”.But the idea was correct.

  • 15Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    “Discovery” of Dark MatterFritz Zwicky (1933)

    Fritz Zwicky (1898 - 1974)

    F. Zwicky, "Die Rotverschiebung von extragalaktischen Nebeln", Helvetica Physica Acta 6: 110–127 (1933)

    F. Zwicky, "On the Masses of Nebulae and of Clusters of Nebulae", Astrophysical Journal 86: 217 (1937)

  • 16Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Rotation Curves of Galaxies

    M(r) increases proportionally to r even beyond the visible edge of the galaxy!

    – hints to presence of large amount of invisible mass beyond the visible galaxy.

    Vera Rubin (1928 - 2016)

  • 17Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Density fluctuations grow too little too late without non-baryonic Dark Matter

    (Source: Web)

  • 18Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Growth of fluctuations and formation of galaxies/clusters

    (Source: Web)

  • 19Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Cosmic Microwave Background

    ● The most perfect Blackbody ever known and measured

    ● Temperature fluctuations carry info about the total amount of matter and amount of baryonic matter in the Universe

  • 20Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Other evidences

    ● (Strong) Gravitational lensing ● Bullet cluster● . . .

  • 21Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    “Bullet cluster”: Collision of clusters of galaxies

    Images: NASA

  • 22Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Planck 2015

    Parameters of the Universe

  • 23Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Dark Matter in the Milky Way (“The Galaxy”)

    ● Rotation curve● Kinematics of vertical motion of disk stars● Dynamics of the globular clusters and dwarf spheroidal satellites of the

    Milky way ● High velocity stars ● . . .

  • 24Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    (Re)constructing the RC of Milky WayFor a particle in a circular orbit

    * Measure v_c(r), get total M(r). Not so simple!

    * Stars on the disk have approximately circular orbits. But stars beyond the disk (> 30 kpc) have non-circular orbits. Also, there are not many tracer stars beyond the disk. Use 21cm line emission from atomic H as tracer.

    *Also, you only measure the line-of-sight component of the velocity.

    *Thus the RC, is not directly measured.It has to be (re)constructed from l.o.s. velocity data

  • 25Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Rotation Curve of the Milky Way

    PB, S.Chaudhury, S. Kundu, ApJ (2014)

  • 26Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Dark Matter in the Galaxy

    PB, S.Chaudhury, S. Kundu (2017)

  • 27Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Dark Matter Density near the Solar System

  • 28Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Candidates for Dark Matter

  • 29Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Can Dark Matter in the Galaxy's Halo be some too-faint-to-see compact objects, such as stellar mass Black Holes, Neutron Stars, Planets (like Jupiter), PBHs?

    MACHOS (Massive Compact Halo Objects)?

    MACHOS can do gravitational microlensing – temporary brightening of stars

    Probability of microlensing 1 in million years per star

    Observe millions of stars

    Only a small fraction of DM as MACHOs allowed (depends on the total halo mass)

  • 30Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Fundamental particle candidates of DM

    ● Weakly Interacting Massive Particles (WIMPs)● Axion-like particles (ALPs)● . . .

  • 31Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    The WIMP `Miracle'DM must be non-baryonic, and can have only very weak interaction with SM particles

    Clustering on (sub)Galactic scales => 'cold', i.e., massive, and hence non-relativistic

    Weakly Interacting Massive Particles (WIMPs)

    In the sufficiently early universe, WIMPs would be in

    thermal equilibrium due to thermal production by

    collision of, and annihilation into, SM particles:

    In thermal equilibrium,

    If thermal equilibrium prevailed till today, present-day abundance would be negligible! But, ...

  • 32Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    The WIMP Miracle …

    Annihilation rate

    since

    But expansion rate So, at some T=T_f, at which

    the species “freezes out” or “decouples” and leaves the exponentially falling abundance curve

    Present -day abundance:

    (Details in Tutorial)

  • 33Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

  • 34Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

  • 35Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Direct detection : Order-of-magnitude estimates

  • 36Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

  • 37Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

  • 38Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

  • 39Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

  • 40Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

  • 41Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    (From: PB, S.Chaudhury, S. Kundu, S. Majumdar, PRD (2013))

  • 42Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

  • 43Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Annual Modulation:DAMA Expt.

  • 44Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Detection Strategies

    The energy deposited by WIMP-induced nuclear recoil in the detector medium manifests as light (scintillation), sound (acoustic waves/phonons) and charge (ionization)

  • 45Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

  • 46Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Background Signal

    Signal and Background

  • 47Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Go Underground to reduce Cosmic Ray Background

    J. Formaggio and C. Martoff, Ann. Rev. Nucl. Part. Sci. 54 (2004) 361

  • 48Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Exclusion Curves (spin-independent interaction)

    Row 1 Row 2 Row 3 Row 40

    2

    4

    6

    8

    10

    12

    Column 1Column 2Column 3

    P. Cushman et al, arXiv:1310.8327

  • 49Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Exclusion Curves: Spin-independent interactions

    Aprile et al (XENON100) 2013

    Xenon1T collab. PRL 119 (2017) 181301 PandaX-II collab. PRL 119 (2017) 181302

  • 50Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Exclusion Curves: Spin-dependent interactions

    Amole et al (PICO) PRL 2015Aprile et al (XENON100) 2013

    (SINP)

  • 51Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    INDIRECT DETECTION

    AMS-02: Positron excess in Galactic CRFERMI-LAT: Gamma rays from WIMP annihilation in dwarf Spheroidal satellites of Milky WaySuper-K, ICECUBE: Neutrinos from WIMP annihilation in Sun…

  • 52Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Whither WIMP Direct Detection?

    Courtesy: Viktor Zacek (adapted from R. Gaitskell)

  • 53Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Ultimate Background: The Neutrino “Floor”

    Cushman et al, arXiv:1310.8327

    DM detectors will start detecting astrophysical neutrinos through Coherent Neutrino-NucleusElastic Scattering (SM process)!

  • 54Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Detecting SN neutrino with DM detectorsusing Coherent neutrino-nucleus Elastic Scattering

  • 55Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    ● Use scintillator crystal as detector material

    ● Proposed to be done in 2 stages :

    – MiniDINO : 1 ---> 10 kg active mass expt. at UCIL Jaduguda mine (SINP, UCIL, BARC, NISER, TIFR, VECC, …. )

    – DINO : > 100 kg expt. @ future INO cavern

    Dark-matter at INO (DINO)

  • 56Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Jaduguda Underground Science Laboratory (JUSL) (Inaugurated on September 2, 2017)

    For carrying out background studies towards a Dark Matter (or other rare event) search experiment

  • 57Pijushpani Bhattacharjee 15 Nov 2017SERC School-EHEP, NISER

    Rig Veda (1st Millenium B.C.)

    THANK YOU !

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