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06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
What’s New in Nu-clear Physics
Ed V HungerfordUniversity of Houston
According to Pogo:
“Nuclear Physics is not
so new, and not so clear
either.”
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
The Answers to our questions are only as good as the questions
themselves
Why did the tree grow in the notch in the fence ?
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
75 years ago Nuclear Physics was New
•The neutron had just been discovered•The Proton and Neutron were considered elementary particles•The nuclear force was not understood•Nuclear models were primitive and based on classical liquids
Today Nuclear Physics in some sense is Mature
•Nucleons are not “elementary” but are composed of other particles called quarks•The nuclear force is understood as an exchange of field quanta called gluons•The nucleus is a VERY complicated interaction of many hadrons whose interaction is described by a theory called Quantum Chromodynamics
Nuclear P
hysics i
s the S
tudy o
f the e
ffects o
f
Many-body H
adronic
System
s inte
ract
ing
via Q
CD
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
The Particles and Symmetries of the Standard Model
3 Families
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
There are 4 known interactions in nature•One of the fundamental driving philosophies of physics is the assumption that these interactions can be “unified” •Two of these are manifestations of the same force (electroweak)•QCD is patterned after the electroweak interaction (gauge theory)•Gravity still lies outside a quantum theory•The new discovery of Dark Energy, if it is real, may imply a 5th force
FieldQCD
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
A Field Quanta
The interaction of B withA occurs through theabsorption of field quantaat B produced by A
Particle B
Particle A
The Interaction through Fields
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
QCD Features
• An interaction that becomes stronger the greater the distance and the lower the energy between interacting particles• A weak interaction at short distances and high energies • A permanently bound quarks and gluons• A self interaction between the field quanta (gluons)• A highly non-linear theory greatly complicating calculations and making intuitive predictions difficult• A symmetry of SU(3) expressed by 3 states of quarks and Gluons (color)
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
Gluon Field
The Quark and Gluon Constituents of the Baryon
Valence Quarks
Sea Quarks
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
Quantum ChromoDynamics (QCD) is the Theory of the Strong Interaction
(Nuclear Force)
Quarks and Gluons
Flux Tube Linear Potential vs distance
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
How do we probe a Nucleon or a NucleusTo determine its Quark Content ?
Incident Electron
Incident Hadron
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
Emission of a Quark Stretches the “interaction String”
When the string breaks, Quark-anti-quark pairs are produced
This is called Hadronization ofa Quark Jet
Quark Scattering
Long Range Nuclear forceCollapses to quark-antiquarkExchange (Yukawa Interaction)the “interaction String”
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
Chiral Symmetry, and Mass
Chiral symmetry is the fundamental symmetry of QCD
But the particle must not have mass
Right HandedVelocity
Left HandedVelocity
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
The QCD Condensate
Particles acquire mass through their interaction with the vacuum, i.e. the condensate of quarks and gluons in the vacuum
A nucleon in a simple visualization, is a bubble in the vacuum condensate
Interaction of these quarks with the condensate at the bubble surfacegives an “effective” mass to the system.
Chiral Symmetry is then said to be spontaneously broken
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
The Vacuum is NOT Empty
This Computer simulationshows the instantaneous gluon field that might be Present in a vacuum. Red Indicates bending(winding) in the field lines perhaps a precursor to quarkcondensates
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
We Live Here
Phase Diagram of Matter
Each of the 4 interactions is has its own impact on the existence of our Universe
The Strong (nuclear) force is responsible for the creation and stability nuclear matter
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
Studying the Vacuum and QCD
RelativisticCollidingNuclei
Quark Gluonplasma
Hadronization
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
Connecting the very large to the very small
One of the more recent advances in physics has been to connect microscopic theory to macroscopic(cosmology)
For example, stellar burning and supernovae produce the nuclei of which the Universe is composed
We can use this information to look back in time, as well as discussthe present features in ouruniverse
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
Mesons and baryons are composed of quarks
Flavor SU(3) SymmetryAllows Placement of lowest MesonsAnd Baryons in Symmetry Octets
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
The Nuclear Equation of State
Neutron Star
Nuclear Matter
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
A modern cut-away view of a Neutron Star
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
Measuring Matter Creation in the Galaxy
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
Proton number vs Neutron Number Stability
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
The Present Model of a Supernovae
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
Inside a SupernovaInside a Supernova
Dense core
100 km M.
3x107 km
3000 km
n*10 km M
.
>8 M evolves ~107 yrExtreme temp: photodissociates nuclei back to protons, neutrons and alphas.
Neutronisation: p+e- n+e
e++e- + ; + x + x (all flavours equally) ~ few x nuclear
Huge thermal emission of neutrinos ~5-10 seconds
Core bounces
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
Supernovae: Facts and FiguresSupernovae: Facts and Figures Energy release ~3x10Energy release ~3x104646 J (the J (the
gravitational binding energy of gravitational binding energy of the core), in about 10 secondsthe core), in about 10 seconds Equivalent to 1000 times the Equivalent to 1000 times the
energy emitted by the Sun in its energy emitted by the Sun in its entire lifetime.entire lifetime.
Energy density of the core is Energy density of the core is equivalent to 1MT TNT per cubic equivalent to 1MT TNT per cubic micron.micron.
99% of energy released is in the 99% of energy released is in the form of neutrinosform of neutrinos
~1% is in the KE of the exploding ~1% is in the KE of the exploding mattermatter
~0.01% is in light – and that’s ~0.01% is in light – and that’s enough to make it as bright as enough to make it as bright as an entire galaxy. an entire galaxy.
Probably site of the r-processProbably site of the r-process..
¼ MT test (Dominic Truckee, 1962)
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
A Computer model of a Supernovae
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop
A Brief SummaryNuclear Science has tremendous breadth and complexity
After 75 years we have found some to the “right” questions to ask but others remain
I have purposely avoided discussion of the more traditional nuclear studies There are impressive new results and insights into nuclear matter. But these require detailed exposition and are difficult to develop to grasp without some prior knowledge.
As a mature, advanced science, there are significant applications in Including the fields of Medicine, Computing, Industrial Products, Energy, Finance, etc.
More than 50% of the Phd graduates in Nuclear Physics are employed in industry, medicine, and national defense.
Nuc
lear
Phy
sics
is a
vib
rant
, exc
iting
Fie
ld
06-20,200506-20,2005 UH Teacher WorkshopUH Teacher Workshop