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Neutrino Physics AAPT Strand Day NSTA Regional, 2005 Jocelyn Monroe, Columbia University 1. What Is a Neutrino Anyway? 2. The Question Of Neutrino Mass 3. Searching For Neutrino Oscillations 4. Where Are We Now? Neutrinos, they are very


  1. Neutrino Physics AAPT Strand Day NSTA Regional, 2005 Jocelyn Monroe, ν Columbia University 1. What Is a Neutrino Anyway? 2. The Question Of Neutrino Mass 3. Searching For Neutrino Oscillations 4. Where Are We Now?

  2. Neutrinos, they are very small. They have no charge and have no mass And do not interact at all. The earth is just a silly ball To them, through which they simply pass... ...And pierce the lover and his lass From underneath the bed- you call It wonderful; I call it crass. J from ``Cosmic Gall'' by John Updike

  3. They say the sun Is gonna grow someday. Tomorrow It's gonna get real close And burn us all up... ...I can't promise you tomorrow No one has the right to lie. Let me see a show of hands. You can beg and steal and borrow. Tell me the truth now. It won't save you from the sky. What happens if Neutrinos have mass? I can't tell you about tomorrow. I'm as lost as yesterday. In between your joy and sorrow, I suggest you have your say: Here's to the little things...

  4. What Is A Neutrino?

  5. from here to the most fundamental ... Atoms are made electrons whiz around of electrons the nucleus and a nucleus The nucleus is made of protons and neutrons Protons and neutrons are made up of quarks We believe these are point-like “ elementary particles ”

  6. The smaller the particles, the bigger the microscopes... discovery of the nucleus 1 st observation of electrons cathode ray tube discovery of heaviest quark (FNAL) discovery of radioactivity discovery of the lightest quarks (SLAC)

  7. The Standard Model

  8. New Physics (Relatively Speaking) 1900s: e discovered (cathode ray tube) γ interpreted as a particle 1930s: µ discovered (cosmic rays) 1950s: ν e observed (nuclear reactor) ν µ discovered (BNL) 1 st evidence for quarks 1960s: u and d observed (SLAC) s observed (BNL) 1970s: standard model is born c discovered (SLAC, BNL) τ observed (SLAC) b observed (FNAL) 1980s: W and Z observed (CERN) 1990s: t quark observed (FNAL) 2000s: ν τ observed (FNAL)

  9. Quarks: make up protons and neutrons top charm up bottom strange down quarks are very cliquish! they appear in nature only in groups Quarks are the only particles that interact via the strong force proton pion

  10. Neutrinos are appear individually in nature... Leptons : from the Greek, "leptos", first lepton meaning thin... electron to be observed electron neutrino ( ν e ) muon muon neutrino ( ν µ ) Lederman, Nobel 1988 tau most recent lepton tau or, alternatively, to be observed neutrino ( ν τ ) "small change"...

  11. About Neutrinos or " little neutral ones " postulated to exist by Wolfgang Pauli in 1930 in order to explain the missing energy in nuclear beta decay electron protron neutron ν e The "desperate way out" electrically neutral weakly interacting extremely light or perhaps massless

  12. The weak interaction is peculiar ... ν out ν in sometimes what you expect... splat ...and sometimes Charged partner not! particle out! ν in ν e  electron ν µ  muon splat Special feature ν τ  tau of the weak force...

  13. We can only detect charged particles! So in a neutrino interaction, we never see the neutrino, just the charged particles from the interaction Luckily electrons muons and taus... why are the tracks curved? ...all leave ...all leave different tracks different tracks

  14. There are neutrinos everywhere!!! ν s from Supernovae Relic ν s from Big Bang So why don't 10 9 per m 3 we know it ??? Cosmic Ray Showers Neutrino Beams made from Reactors and Particle Accelerators

  15. They call it the weak force for a reason! neutrinos interact 100,000,000,000 times less often than quarks ν ... A neutrino has a good chance of traveling through 200 earths before interacting at all!

  16. ktons You need a lot of neutrinos 100 and a lot of detector 30 Super-K (55 kt) to have any interactions at all! 10 Kamland (3 kt) SNO (1 kt) 3 1 Grand Experiments MiniBooNE (800 t) 0.3 ...for a Petite Particle! 0.1

  17. The Question of Neutrino Mass ?

  18. Neutrinos really are incredibly petite ν e 10 2 1 grams grams grams At least 500,000 times lighter than an electron In the Standard Model neutrinos are massless

  19. What is a massless particle? particles are just bundles of energy E = mc 2 + K Energy of motion The photon is an example of a massless particle. Massless particles always travel at the speed of light. If the data are consistent with neutrinos being massless, and the theory is very tidy if neutrinos are massless...

  20. Therefore... The Standard Neutrinos Model says have no neutrinos are mass! massless. Or do they?

  21. And for a long time everything seemed fine we were until we observed a Quantum Mechanical wrong! phenomenon that told us

  22. about waves Waves have periodic motion: f(x,t) = A sin (kx - ω t) x (space): amplitude = A wavelength λ = 2 π / k λ A t (time): period T = 2 π / ω velocity v = ω / k v frequency of repetition in time = ω / 2 π frequency of repetition in space = k / 2 π

  23. superpositions of waves If you add two waves (or more) you will get another wave = + Lots of waves have multiple components: e.g., Musical Chords, Neon Lights

  24. if the components are similar... ● take one wave ● add one of similar frequency ● sum exhibits interference: this phenomenon is called “ beats ” Musical beats occur when a tiny physical difference between two tuned instruments causes a slight difference in frequency

  25. more on beating this is like adding 2 waves and getting 2 waves out: f(x,t) = f 1 (x,t) + f 2 (x,t) = 2A sin(K x - Ω t) cos(k x - ω t) a wave with the average frequency of the first 2 k = ½ (k 1 + k 2 ), ω = ½ ( ω 1 + ω 2 ) AND a ''beat wave'' with the beating frequency K = ½ (k 1 - k 2 ), Ω = ½ ( ω 1 - ω 2 )

  26. waves & particles Quantum Mechanics: particles act like waves of wavelength λ = (Planck's constant / momentum) -de Broglie, 1924 massive particles: momentum = mass x velocity massless particles: momentum = energy / c c = speed of light in vacuum = 3 x 10 8 m/s particles can be superpositions of waves too! 1927 Solvay Conference participants, ''founders of Quantum Mechanics''

  27. neutrino oscillations are beat waves ν µ ν µ ν µ ν µ The initial neutrino flavor fades and returns ν e ν e ν e ν e & when the initial flavor fades a new flavor shows up...

  28. This can only happen if the neutrino wave is made of two waves, with a small wavelength difference causing the “ beats ” . .. and that difference is mass. In other words: if we see neutrino oscillations, it requires that neutrinos have mass.

  29. neutrinos drive supernovae explosions Even a tiny mass can change the way the universe works neutrinos power the sun radioactivity heats the earth's core, which moves neutrinos tectonic plates may be a component of dark matter

  30. How to Search for Neutrino Oscillations

  31. 2 L 2 2  sin 2  1.27  m P  a  b = sin E  Oscillation probability between 2 flavor states depends on: 1. fundamental parameters ∆ m 2 = m 1 2 -m 2 2 = mass difference between states sin 2 2 θ = mixing between ν flavors Pontecorvo, 1957 2. experimental parameters L = distance from ν source to detector E = ν energy ν ν ν ν ν ν ν ν ν ν ν ν ν ν ν ν ν ν ν ν ν ν

  32. Two things can happen between production and detection of a neutrino beam: (fix E, let L vary) 1. neutrinos of the flavor you start with disappear 2. neutrinos of the flavor you didn't start with appear

  33. Oscillations change both the number and the energy spectrum of the neutrino beam: (fix L, let E vary) # ν e # ν µ Appearance Disappearance Expected Detected Detected Expected ν e Energy ν µ Energy

  34. Detecting Neutrinos Seeing neutral particles is really hard, but when ν s interact via the ``Charged Current Interaction,'' a ν goes in, and its charged partner particle comes out Special feature Charged partner of the weak force... particle out! ν in ν e  electron ν µ  muon splat ν τ  tau target nucleus ...by observing the charged particle partner, one can infer the neutrino flavor

  35. Detecting Charged Particle Partners W a v e f r o n t Charged particles passing through material can produce visible light via Cherenkov radiation Particle track Light emitted by material if particle v > c / n θ C Similar to a sonic boom

  36. Example: the MiniBooNE Detector 4-story tall spherical tank, filled with oil, lined with photo-multiplier tubes (PMTs) PMT PMTs detect photons from ν -interaction induced light emission in oil, record time of arrival and number of photons Reconstruct particle tracks from time and angular distributions

  37. Photo-Multiplier Tubes light in, current out Photon liberates electron negative via potential photoelectric effect electron signal read out a current, amplified up to tells you how much 10 8 electrons light hit PMT number of photons = 10 -8 x number of electrons out

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