0 Neutrino Conversations Boris Kayser NeutrinoFest April 18, 2005.

Slides:



Advertisements
Similar presentations
"Now I am become Death, the destroyer of worlds." Robert Oppenheimer after the first test of the atomic bomb.
Advertisements

Einstein’s Energy Mass Equivalence Powers the Sun!
Neutrinos 2. Neutrino scattering
1 Neutrino Phenomenology Boris Kayser Scottish Summer School August 9,
Big Bang …..was actually very small and quiet. Atoms are mostly empty space.
Nuclear Physics UConn Mentor Connection Mariel Tader.
“The Story of the neutrino” Does the missing matter matter? or.
Atmospheric Neutrino Anomaly
8/5/2002Ulrich Heintz - Quarknet neutrino puzzles Ulrich Heintz Boston University
Neutrinos and SN1987A Brent Tunis. What exactly are Neutrinos? Neutrinos were formally discovered by Enrico Fermi in 1934 when he realized that, in order.
Modern Physics LECTURE II.
Neutrino emission =0.27 MeV E=0.39,0.86 MeV =6.74 MeV ppI loss: ~2% ppII loss: 4% note: /Q= 0.27/26.73 = 1% ppIII loss: 28% Total loss: 2.3%
Fusion Energy. Source of Energy Before 1940 the Sun’s energy was a mystery.  Chemical reactions:  Gravitational energy:  Nuclear forces: The Sun is.
Nuclear Force and Particles
Modern Physics Introduction To examine the fundamental nuclear model To examine nuclear classification To examine nuclear fission and fusion.
Fundamental Particles (The Standard Model) Nathan Brown June 2007.
Particle Physics Intro. What’s Stuff Made Of…Really? All particles can be grouped into two categories: Fermions and Bosons Things to know about Fermions:
UPRM Center Rafael Aramis López LEAD TEACHER. The Universe is made of Quarks and Leptons Everything from galaxies to mountains, to molecules is made from.
Dark Matter Masses of Galaxies Gravity and Light Black Holes What is Dark Matter?
Anatomy of a collider detector Silicon vertex detectors- small but important.
Goal: To understand the lifetime of a star and how the mass of a star determines its lifetime Objectives: 1)To learn what defines a Main sequence star.
The Particle Zoo. Too Many Particles Far from just finding Protons Neutrons Electrons Neutrinos and their antiparticles, during the 20 th century many.
Section 1: Structure of the Sun
Particle Physics J4 Leptons and the standard model.
My Chapter 30 Lecture.
0 American Physical Society MultiDivisional Neutrino Study DOE-OS Briefing January 7, 2005 Washington DC Stuart Freedman Boris Kayser.
Point 1 activities and perspectives Marzio Nessi ATLAS plenary 2 nd October 2004 Large Hadron Collider (LHC)
The Elementary Particles. e−e− e−e− γγ u u γ d d The Basic Interactions of Particles g u, d W+W+ u d Z0Z0 ν ν Z0Z0 e−e− e−e− Z0Z0 e−e− νeνe W+W+ Electromagnetic.
0 Physics of Neutrinos From Boris Kayser, Fermilab.
Finishing things up. So what’s with that 14 C? Masses of isotopes (not “natural” stuff) truly are multiples of basic hydrogen. Hydrogen is positively.
Nuclear Forces The power behind Stars. Fundamental Forces Gravity –Attractive force governed by mass Electromagnetism –Attractive or repulsive force that.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 30: Particle Physics Fundamental.
Wednesday, Feb. 14, 2007PHYS 5326, Spring 2007 Jae Yu 1 PHYS 5326 – Lecture #6 Wednesday, Feb. 14, 2007 Dr. Jae Yu 1.Neutrino Oscillation Formalism 2.Neutrino.
A singularity formed by a previous collapsed Universe? Multiple Universes? We just don’t know… YET What Caused It?
Neutrino Nobel Prize overview
1 Neutrino Phenomenology Boris Kayser Scottish Summer School August 11,
The Heart of the Sun Energy Generation in Sun-like Stars.
Chapter 17 The Beginning of Time. Running the Expansion Backward Temperature of the Universe from the Big Bang to the present (10 10 years ~ 3 x
The Nucleus Nucleons- the particles inside the nucleus: protons & neutrons Total charge of the nucleus: the # of protons (z) times the elementary charge.
On 4 December 1930, Austrian theorist Wolfgang Pauli (pictured here in 1933) wrote a famous letter in which he dared to hypothesise the existence of new.
Neutrinos: What we’ve learned and what we still want to find out Jessica Clayton Astronomy Club November 10, 2008.
What IS Fundamental???  Many new particles were discovered with the advent of particle accelerators …are they ALL fundamental??? Baryons: particles with.
Quarks and Leptons Announcements 1.Recitation this week in lab. BRING QUESTIONS ! 2.See my by Wed. if you have any grading issues with your exam. 3.Reading.
Modern Physics. Reinventing Gravity  Einstein’s Theory of Special Relativity  Theorizes the space time fabric.  Describes why matter interacts.  The.
Introduction to Particle Physics (for non physics students) 2. PARTICLES (from atoms to quarks and leptons)
Goal: To understand the history of the universe especially the beginning Objectives: 1)To learn about the beginning of the Big bang! 2)To explore the Big.
Take out hwk & tables. Compare answers to hwk sets.
Solar Neutrinos By Wendi Wampler. What are Neutrinos? Neutrinos are chargeless, nearly massless particles Neutrinos are chargeless, nearly massless particles.
1 The Standard Model of Particle Physics Owen Long U. C. Riverside March 1, 2014.
What makes up the nucleus? Nucleus is positively charged Different atoms have same electrical properties but different masses Isotopes – same atomic number,
Particle Detectors January 18, 2011 Kevin Stenson.
Sun Nuclear Reactions If the mass in the center of the solar nebula is large enough, gravity will collapse more and more material, producing higher and.
Neutrino. Game Board FERMILABHAPPENINGSFIRSTSNEUTRINOSDETECTION.
CHAPTER 14 Elementary Particles
PHL424: 4 fundamental forces in nature
Neutrino Oscillations and T2K
Neutrinos and the Evolution
The Physics of Neutrinos
HCP: Particle Physics Module, Lecture 4
Non-Standard Interactions and Neutrino Oscillations in Core-Collapse Supernovae Brandon Shapiro.
The Beginning of Time (Birth Of The Universe)
PHL424: 4 fundamental forces in nature
Pauli´s new particle * nt nm ne e m t Beta-Decay Pa 234 b (electron)
What’s the matter with antimatter?
The Neutrino World: Present and Future Boris Kayser
1930: Energy conservation violated in β-decay
Particle Physics Lesson 6
Fundamental Particles
Neutrino JEOPARDY!.
Presentation transcript:

0 Neutrino Conversations Boris Kayser NeutrinoFest April 18, 2005

1 The Universe and Us It used to be thought that —

2 Our home planet—

3 — is the center of the universe. But we now know that the address of our home planet is — #3 No-Place-Special Street.

4 We, and all everyday objects, are made of 3 kinds of tiny particles: These are bundled together to make Atoms: ElectronsNeutronsProtons Proton Neutron Electron

5 It used to be thought that the Whole Universe is made of the same particles as we are: Electrons Protons Neutrons But we now know that in the universe as a whole, these particles are rareties. For every electron, proton, or neutron, the universe contains over a billion neutrinos.

6 Together with photons (the particles of light), neutrinos are by far the most abundant particles in the universe. To understand the universe, we must understand the neutrinos.

7 Are Neutrinos Important to Our Lives? If there were no s, the sun and stars would not shine. No energy from the sun to keep us warm. No atoms more complicated than hydrogen. No carbon. No oxygen. No water. No earth. No moon. No us. No s is very BAD news.

8 Getting Acquainted With Neutrinos neu  trï´no: Little neutral object Enrico Fermi Q : How little are neutrinos? A: About the same size as electrons. Roughly 1/10,000,000,000,000,000 inch across. This is 1/1,000 the size of an atomic nucleus.

9 Q : How strongly do neutrinos interact with other matter? A: VERY FEEBLY. Every day, 10,000,000,000,000,000,000,000 neutrinos from the sun pass through the Sudbury Neutrino Observatory (SNO), 1000 tons of heavy water in a sphere 40 feet across. Only 10 of them interact. The rest zip right through. BIG detectors are needed to stop and study neutrinos.

10

11 Q: How much do neutrinos weigh? A: Almost nothing. Years of experiments yielded no evidence that neutrinos have any mass at all. Q: Can a particle have no mass at all? A: A particle can be a bundle of pure energy, and have no mass at all. The photon—the particle of light—is like that. But in the last 7 years we have discovered that neutrinos are not like that. They have nonzero masses. However, the mass of each neutrino is less than one-millionth the mass of an electron.

12 Q: Are all neutrinos the same, or are there different kinds of neutrinos? A: Neutrinos come in three different flavors: The electron neutrino e The muon neutrino  The tau neutrino  Q: How do we know neutrinos have masses? A: We’ll explain that shortly.

13 Q : How do e, , and  differ from one another? A: There are 3 kinds, or flavors, of electron-like particles: e, , and  are electrically charged, and are known as the charged leptons. Associated Neutrino e   Particle Symbol Mass Electrone 1 Muon  200 Tau  3500

14 Neutrinos are created in a variety of physical processes. In nature or the laboratory, a neutrino is created together with a charged lepton. The neutrino and charged lepton always have the same flavor.       or Not e e Source

15 When a neutrino collides with an atom in a neutrino detector, it creates a charged lepton. The charged lepton always has the same flavor as the neutrino.      or Not e e Detector e

16 e e Detector e e Source     The flavors match. Creation and Detection of a Neutrino Short Journey

17 The Discovery of Flavor Change The last 7 years have yielded compelling evidence that, given enough time, a neutrino can change from one flavor into another.   Detector   Source Long Journey This is surprising behavior. Once an electron, always an electron. But once a e, not always a e.

18 How We Know Neutrinos Change Flavor In the core of the sun Nuclear Reactions Solar neutrinos are all born as e, not  or . e e — Solar Neutrinos —

19 SNO detects solar neutrinos in several different ways. One way counts Number ( e ). Another counts Number ( e ) + Number (  ) + Number (  ). SNO finds Number ( e ) Number ( e ) + Number (  ) + Number (  ) = 1/3.

20 All the solar neutrinos are born as e. Neutrinos change flavor. But 2/3 of them morph into  or  before they reach earth.

21 — Atmospheric Neutrinos — Cosmic rays come from all directions at the same rate. So atmospheric neutrinos are produced all around the earth at the same rate. But Number (  Up) / Number (  Down) = 1/2. Detector Cosmic ray  

22 Half the  that travel to the detector from the far side of the earth disappear en route. The detailed data show that the disappearance is due to —   

23 Evidence For Flavor Change Neutrinos Solar Atmospheric Reactor Accelerator Evidence of Flavor Change Compelling Strong

24 Neutrino Flavor Change Implies Neutrino Mass The neutrinos we study pass through matter between their source and our detector. Can’t their interactions with the matter change their flavor? In practice, no. We have confirmed that the interactions between neutrinos and matter are very well described by the Standard Model of elementary particle physics. Standard Model neutrino interactions do not change neutrino flavor.

25 Therefore, neutrinos must be changing their flavor on their own. We observe that they do this over time. A has a sense of time. Only particles with mass have a sense of time. Therefore, a neutrino must have a mass.

26 The Physics of Neutrino Flavor Change If particles like the electron never morph into something else, how can a  morph into a  ? Answer: A  is not a particle to begin with. There are neutrino particles: Neutrino Particle Mass m1m1 m2m2 m3m3 (And maybe more.)

27 e, , and  are different MIXTURES of 1, 2, and 3. In each of—     e e the emitted neutrino is actually a 1, 2, or 3.  is: Probability 17 % 34 % 49 % maybe 1 maybe 2 maybe 

28 The world of the subatomic particles is governed by QUANTUM MECHANICS. An object can be maybe here and maybe there. It can be maybe this and maybe that. It can be maybe a 1, maybe a 2, and maybe a 3. Quantum mechanics involves uncertainty at its core.

29     Long Journey Voyage of a Neutrino Original 1, 2, 3 mixture New, different 1, 2, 3 mixture 1, 2, 3 travel differently because they have different masses. The  mixture of 1, 2, 3 has turned into the  mixture. Neutrino flavor change is a quintessentially quantum mechanical phenomenon. It occurs over VERY LARGE distances.

30 The quantum mechanics of flavor change results in an oscillation back and forth between the initial flavor and the new one. Thus, flavor change is called — NEUTRINO OSCILLATION An example, starting with a  :

31 Neutrino Oscillation

32 What We Have Learned

33 The Neutrino Mass Spectrum There are at least 3 neutrino particles: 1, 2, 3. Neutrino oscillation results have revealed the differences between the squares of their masses. The spectrum of squared masses looks like —

34 (Mass) or }  m 2 sol  m 2 atm }  m 2 sol  m 2 atm  m 2 sol =  m 2 atm / 30  m 2 atm = (Electron mass / 10,000,000) 2 Not above (Electron mass / 1,000,000) 2. {From Cosmology}

35 When one of the neutrino particles ( 1, 2, or 3 ) interacts in a detector and makes a charged lepton, this charged lepton could be an e, a , or a . It’s that quantum-mechanical uncertainty again! But, for each neutrino particle, we know the probability that the charged lepton it produces will be of any particular flavor.

The Probabilities of Making e, , and 

37 The Open Questions

38  How many different neutrino particles are there? CERN: If there are more than 3, then at least one mixture of them does not participate in any of the known forces of nature except gravity. All known particles participate in some force besides gravity. e, , and  participate in the weak nuclear force.  An object that doesn’t experience any of the known forces except gravity would be very different. LSND (Liquid Scintillator Neutrino Detector): There are more than 3 neutrino particles. MiniBooNE (in progress): Is the LSND experiment right or wrong?

39  How much do the neutrino particles 1, 2, and 3 weigh? Can we use cosmology? Can observations of the structure of the universe tell us, not just an upper limit on the mass of any neutrino particle, but the actual masses of these particles? Can we use laboratory experiments?

40 Does the neutrino mass spectrum look like or like ? Grand Unified Theories: The neutrinos and the charged leptons are cousins of the quarks. The quark spectra look like. So, if these theories are right, the neutrino spectrum should look like too. To find out if it does, pass a beam of neutrinos through more than 500 miles of earth matter. The behavior of the neutrinos in matter will depend on which kind of a spectrum we have.

41  Are neutrinos identical to their antiparticles? For every particle, there is a corresponding antiparticle. Particle Antiparticle Electron PositronElectric Charge Proton AntiprotonElectric Charge Neutron AntineutronBaryonic Charge Neutrino Antineutrino ?? Difference Matter Antimatter

42 Is there a “leptonic charge” L such that — L( ) = L(e – ) = –L( ) = –L(e + ) = 1 ? That would explain why — e e–e– e e+e+ but But if there is no such leptonic charge, then there is nothing to distinguish a from a.

43 Then, unlike all the other constituents of matter — the charged leptons, and the quarks that make up protons and neutrons — the neutrinos are identical to their antiparticles: =. This would make neutrinos very distintive. How can we confirm that = ? “Charges,” such as the hypothetical leptonic charge L, are conserved quantities: Process L(in) L(out) = L(in)

44 So look for — New Nucleus Nucleus e–e– e–e– Neutrinoless Double Beta Decay (0  ) L = 0 L = 1 Does not conserve leptonic charge L, so =.

45  What is the origin of neutrino mass? Observation of neutrinoless double beta decay would The origin of neutrino mass is different from the origin of the masses of electrons, quarks, protons, neutrons, humans, the earth, and galaxies.

46  Are neutrinos the reason we exist? The universe contains Matter, but essentially no antimatter. Good thing for us: This preponderance of Matter over antimatter could not have developed unless the two behave differently (“CP violation”). A difference not involving neutrinos has been seen, but it is way too small to explain the universe. Matter Antimatter Poof!

47 Does Matter interact with neutrinos differently than antimatter does? Could this difference explain the universe?

48 There is a natural way in which it could. The most popular theory of why neutrinos are so light is the — See-Saw Mechanism N Very heavy neutrino Familiar light neutrino } {

49 The heavy neutrinos N would have been made in the hot Big Bang. Then they would have disintegrated into lighter particles: N  e - + … and N  e + + … Matter antimatter If Matter and antimatter interact differently with neutrinos, both heavy and light, then one of these disintegrations can be more likely than the other. Then we would get a universe with unequal amounts of Matter and antimatter.

50 Can we confirm that Matter and antimatter actually do interact differently with neutrinos? Source Detector e-e- -- Source Detector e+e+ ++ A neutrino flavor change involving Matter : A neutrino flavor change involving antimatter : Do these processes have different rates?

51 we are all descendants of heavy neutrinos If N decays led to the present preponderance of Matter over antimatter, then we are all descendants of heavy neutrinos.

52 Recommendations of the APS Multi- Divisional Study

53 High priority: Searches for neutrinoless double beta decay, to see if =.

54 High priority : A program to —  find out how big the small e-flavored wedge in 3 is  determine whether the mass spectrum looks like or like  search for CP violation in neutrino flavor change CP violation: Neutrinos interact differently with matter than with antimatter. There can be no CP violation unless the pie chart for every neutrino particle involves all three colors.

55 Important : Develop an experiment that can make detailed studies of the neutrinos from the primary fusion process that we think powers the sun. These neutrinos have lower energy than those studied in detail so far. Now that we understand neutrinos much better, we can use them to test whether we truly understand how the sun works.

56 Conclusion There has been an explosion in our knowledge of the neutrinos in the last seven years. The recent discoveries have raised very interesting questions that we must now try to answer. Exciting, challenging, experiments to answer them will be launched in the coming years.