The Spring 2019 unique number is
55590; the class meets from 12 to 1 PM MWF in RLM
5.104. The TA is Josiah Couch.
Office: RLM 9.308. Hours: 9-10 AM on Mondays and
Wednesdays.
Text: SUBATOMIC PHYSICS, 3rd
Edition, by Henley
and Garcia
(World Scientific, 2007, 2010). Errata
for Ch. 6, and
errata for Ch. 11. [I have located a
free pdf version of the text, here.]
And here
is a very compact introduction to the theory of
scattering. A
short course in nuclear physics. Highly
recommended supplementary text: PARTICLES AND
NUCLEI, 7th edition, by Povh, Rith, Scholz,
Zetsche and Rodejohann (Springer, 2015). The only
reason I don't use this as the primary text is that
it has no homework problems.
Syllabus
and first day handout. Basis of course letter
grade: Homework 85%, daily pop quizzes 15%.
Other books on course topics:
Particle Physics in the LHC Era, by
G. Barr, R. Devenish, R. Walczak and T. Weidberg,
Oxford, 2016.
Modern Particle Physics, by M. Thomson,
Cambridge, 2013.
Particle Physics, by D. Carlsmith,
Pearson, 2013.
Nuclear Physics in a Nutshell, by C.
A. Bertulani, Princeton, 2007.
Basic Ideas and Concepts in Nuclear Physics,
by K. Heyde, 3rd Ed., IOP London, 2004.
An Introduction to Nuclear Physics,
by W. N. Cottingham and D. A. Greenwood, 2nd Ed.,
Cambridge, 2001.
Introductory Nuclear Physics, by P.
E. Hodgson, E. Gadioli and E. Gadioli Erba, Oxford,
1997.
RUNNING TABLE OF HOMEWORK DUE
DATES AND TIMES: HW
1 statistics: 18 students turned in the
assignment. High grade 91%, low grade 45%, average
75%. HW
2 statistics: 22 students turned in the
assignment. High grade 100%, low grade 0%, average
67%. HW
3 statistics: turned in by 22 students.
Highest grade 93%, lowest grade 62%, average grade
73%. HW
4 statistics, high grade 97.5%, low grade 19%,
average 80%, turned in by 20 students. HW
5, due in class on March 27.
HW 6, due in class on April 3. HW7,
due in class April 10.
Answers to in-class
quizzes: (1) The Feynman diagram is for pair
creation. Since the photon is massless and the
electron and positron have a mass of 0.5 MeV, total
energy and momentum can't be conserved unless
another massive object (the nucleus of a heavy atom)
is also involved in the initial state of the
process. (2) Clearly a system made of a
particle and an antiparticle is not going to be
stable. What's astonishing is that all
strongly-interacting composite particles can be put
into two groups, baryons and mesons, and it turns
out no meson is stable, and only one baryon seems to
be stable, the proton. (3) Typical average
lifetimes: strong processes, 10−23 sec;
electromagnetic processes, 10−17 sec;
weak processes, 10−10 sec, as you would
expect. (4) The neutral D decay involves a W+ boson,
the gauge boson of the weak force. (5) Isospin
obeys the same rules as angular momentum, so isospin
T results in a 2T+1 multiplet. Since 2T+1 = 5, T =
2. (6) The Poynting Vector is a cross product
of a polar vector E and an axial vector B. So
it transforms like a polar vector. PS = -SP. (7)
Photons emitted by pointlike fundamental particles
are virtual. (8) A negative pion decaying to a
muon and an anti-muon-neutrino is of course a
semi-leptonic process. (9) ALL of the
statements about the weak interaction are
correct. (10) The original quark model (1961)
used only 3 quarks, u, d and s. (11) The
spectra of 64Zn and 122Te
exhibit the classic pattern of vibrational nuclei...
a one phonon (λ = 2) state and then a triplet
indicating excitation of two coupled λ = 2 phonons.
If you missed this straightforward question, take it
as a warning that you are not now keeping up in the
class or comprehending even very basic
material. (12) If a nucleus has a half-life of
one day, and at some point a sample contains 10,000
such nuclei, one day later there will be
5,000. (13) 48% comes from diagnostic
X-radiation, and 37% from radioactive gases emitted
by subsequent decays of naturally-occurring U and Th
in dirt and rocks. (14) Fission releases a
kinetic energy of about 1 MeV per nucleon, 200 MeV
total. (15) The first physicist to suggest
that the chemical elements were forged by nuclear
processes in the cores of stars was Sir Arthur
Eddington. When other physicists expressed
skepticism, Sir Arthur would always reply, "Then why
don't you go find a hotter place?" (16) The
first physicist to realize that the universe must
have started out in a very hot, extremely dense
state (and to estimate a value of the Hubble
constant before Edwin Hubble even discovered the
expansion of the universe observationally) was
Georges Lemaître. (17) Only about 4% of our
universe consists of ordinary matter--- electrons,
protons, neutrons (in nuclei), neutrinos and
photons. (18) It's pretty much universally
agreed now that the idea of supersymmetry
is incorrect.
Course notes: Part
1,
Part 2, Part
3,
Part 4,
Part 5, Part
6,
Part 7,
Part 8,
Part 9,
Part 10. Notes for the last few weeks
of the course are entirely on the web pages
projected during the class lectures.
CLASS SLIDES FOR 362L: Accelerators
& relativity, Diagrams,
cross
sections, Running
coupling constants,
Particles,
Observing,
Symmetry,
Isospin,
PCT,
EM radiation,
Weak 1, Gauge
Symmetry, Electroweak1,
Strong1, Supersymmetry?
Quarkonium,
Valence
Quarks, FermiGas,
IMP,
Optical Model,
Heavy ions, Direct
Reactions,
Mass Formula, Nuclear
Vibrations,
Nuclear Rotations,
The Little Bang,
Unstable Nuclei, Radiation,
Power,
Fusion, Stars,
Evolution,
Late Stages, Nucleosynthesis,
Pioneers,
Cosmology,
The
Big Flash!
Dark Matter,
Matter Origins,
Dark Energy,
Inflation,
When Chiral Symmetry Breaks, Strings,
Black Hole History,
Black Hole Primer,
Quantum Gravity?
Loop Quantum Gravity,
CDT-CS,
Frontiers? [The remaining two links were not
used in this class.]
Unused 1,
Unused 2
CLASS SLIDES FOR
302L:
Relativity 1,
Relativity 2,
Twins!
Length Contraction!
Binding Energy,
Einstein's Theory of Gravity,
Quantum 1,
Quantum 2,
Atoms,
Spin and Pauli Principle,
Molecules and Solids,
X rays and Lasers,
Nuclear1,
Nuclear2,
Radiation,
Fission and Fusion,
The Sun,
Particles!
The Proton, Early
Universe, THE
DARK!

Einstein
No
fairer destiny could be allotted to
any physical theory, than that it
should of itself point out the way to
the introduction of a more
comprehensive theory, in which it
lives on as a limiting case. [From his
1920 book summarizing the Special and
General Theories of Relativity]
|
In Spring 2019, watch
for the Pizza
Seminar! ♣
Coker's Homepage
♥
|

Bose
|

Fermi
Before I
came to the conference, I was confused
about this subject. Having listened to
your lecture, I am still confused. But
on a higher level. [Fermi to a
conference speaker.]
|

Dirac
The
steady progress of physics requires
for its theoretical formulation a
mathematics which get continually more
advanced. This is only natural and to
be expected. What however was not
expected by the scientific workers of
the last century was the particular
form that the line of advancement of
mathematics would take, namely it was
expected that mathematics would get
more and more complicated, but would
rest on a permanent basis of axioms
and definitions, while actually the
modern physical developments have
required a mathematics that
continually shifts its foundation and
gets more abstract. Non-euclidean
geometry and noncommutative algebra,
which were at one time were considered
to be purely fictions of the mind and
pastimes of logical thinkers, have now
been found to be very necessary for
the description of general facts of
the physical world. It seems likely
that this process of increasing
abstraction will continue in the
future and that advance in physics is
to be associated with continual
modification and generalisation of the
axioms at the base of mathematics
rather than with a logical development
of any one mathematical scheme on a
fixed foundation. [Paper on Magnetic
Monopoles (1931)]
|

Feynman
Trying
to understand the way nature works
involves a most terrible test of human
reasoning ability. It involves subtle
trickery, beautiful tightropes of
logic on which one has to walk in
order not to make a mistake in
predicting what will happen. The
quantum mechanical and relativity
ideas are examples of this.
|

Gell-Mann
In our
work, we are always between Scylla and
Charybdis; we may fail to abstract
enough, and miss important physics, or
we may abstract too much and end up
with fictitious objects in our models
turning into real monsters that devour
us.
|

Weinberg
I do
not think it is possible really to
understand the successes of science
without understanding how hard it is
[to do science]— how easy it is to
be led astray, how difficult it is
to know at any time what is the next
thing to be done.
|

Salam
From
time immemorial, man has desired to
comprehend the complexity of nature in
terms of as few elementary concepts as
possible.
|

Witten
In Newton's
day the problem was to write something which
was correct --- he never had the problem of
writing nonsense, but by the twentieth
century we have a rich conceptual framework
with relativity and quantum mechanics and so
on. In this framework it's difficult to do
things which are even internally coherent,
much less correct. Actually, that's
fortunate in the sense that it's one of the
main tools we have in trying to make
progress in physics. Physics has progressed
to a domain where experiment is a little
difficult... Nevertheless, the fact that we
have a rich logical structure which
constrains us a lot in terms of what is
consistent, is one of the main reasons we
are still able to make theoretical advances.
Two Pb
nuclei collide at 160 GeV per nucleon.
|