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Physics Beyond the Standard Model

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Title: Physics Beyond the Standard Model


1
Physics Beyond the Standard Model
  • Summary by Dennis Silverman
  • Physics and Astronomy
  • UC Irvine

2
Where Does Mass Come From?
  • The electroweak gauge theory only has conserved
    currents for its weak charges if the Ws and Z
    are massless, like the photon is. It also helps
    if quarks and leptons are massless in the Energy.
  • To maintain this, but yet have physical masses,
    we fill the vacuum with some sludge. A
    particles mass is then proportional to the
    amount each particle couples to this sludge.
  • The sludge is the everywhere constant vacuum
    value of the neutral Higgs.

3
The Higgs Fields in the SM
  • Three extra Higgs fields, H, H-, anti-H0 make up
    the extra component of the W and Z spins needed
    to make them massive.
  • The Ws have a mass of 81 GeV, and the Z of 90
    GeV.
  • The H0 has a constant vacuum density, and can
    also make a physical particle.

4
How to Find the Higgs
  • The Higgs vacuum value is uniform, neutral,
    appears the same at all velocities, and
    undetectable except for the fact that it gives
    mass to everything.
  • A particles mass is proportional to its coupling
    to the Higgs and therefore to its vacuum density.
  • The excitations of the Higgs is a real particle,
    predicted to be at about 115-130 GeV.
  • This should show up in the LHC in some rare
    decays.
  • It would have shown up at the Fermilab Tevatron,
    except that the intensity has not met
    expectations.

5
Increasingly General Theories
  • Grand Unified Theories of electroweak and strong
    interactions
  • Supersymmetry
  • Superstring Theories 10 dimensions with gravity
  • Superstring Unification to M Theory

6
Running Coupling Constants
  • Charged particles have virtual quantum allowed
    clouds around them of photons and
    electron-positron pairs.
  • Colored particles have virtual gluons and
    q-anti-q pairs.
  • So the total coupling at long distance or
    charge, is different from the coupling at short
    distance, where the the cloud is penetrated.
  • Electromagnetic coupling ?1 e2/?c increases
    with energy from 1/137 to 1/40 at 1017 GeV
    Unification Scale
  • Strong coupling ?3 g2/?c decreases from 1 to
    1/40
  • Weak coupling to Ws is ?2.
  • So couplings come together at unification scale

7
Running Gluonic Coupling
g3
g3
?3 (g3)2 /?c
8
Running Couplings
9
Fundamental Particles for Unification
  • Unification means that at a GUT scale, where
    masses can be ignored, all fundamental particles
    appear in the same multiplet.
  • This allows their charges to be the same or given
    fractions of each other, and accounts for the
    proton and electron charge being equal.
  • The particles from the SM to include for the
    first generation are the 16 (left handed)
  • ur ug ub dr dg db anti-(ur ug ub dr dg db)
  • ?e e- anti-?e e
  • Recently, neutrino oscillations and mass were
    found, adding the anti-?e.
  • In the GUT, there are vector bosons that take
    fundamental particles into another in the
    multiplet.

10
Sequence of GUTS
  • Standard Model of electroweak doublets for quarks
    and leptons plus photon (SU(2)xU(1)) and three
    colors (xSU(3)). It has ?, W, Z, and 8 gluons
    as bosons.
  • Combine 3 colors and electroweak doublet (SU(5))
    ruled out as causes proton decay at level not
    seen has 5 10 fundamental particles. It has
    24 bosons.
  • Add extra neutrino mode for massive neutrinos
    16 fundamental (SO(10))
  • There are 45 gauge bosons in SO(10).
  • 27 fundamentals (E6), including singlet quarks
    and neutrinos.
  • E7, E8 (heterotic string)
  • Three generations of each fundamental multiplet

11
A Bit of History of Unification
  • Electricity unified with magnetism (M. Faraday
    and J. C. Maxwell).
  • Relativity and General Relativity (A. Einstein).
  • Quantum Mechanics (Planck, Bohr, Schrodinger and
    Heisenberg).
  • Relativistic quantum mechanics (P. Dirac).
  • Quantum Electrodynamics (R. Feynman, Tomonaga,
    Schwinger).
  • Quarks and Quantum Chromodynamics (Nemann, M.
    Gell-Mann and G. Zweig).
  • Unification of Electromagnetism with Weak
    Interactions to form Electroweak theory (S.
    Weinberg, A. Salam).
  • Grand Unified Theories
  • Supersymmetry
  • Superstring Theory of Everything including
    gravity.

12
Proton Decay
  • In a GUT there are X and Y gauge bosons that can
    transform a quark into an antiquark, and a quark
    into a lepton, since they are in the same
    multiplet.
  • This allow protons in quarks to decay into a
    lighter pi or K meson and a lepton.
  • Dont worry, the lower limit on the lifetime is
    1034 years, far longer than the age of the
    universe of 1010 years.
  • It takes a detector the size of Super-K to see a
    few proton decays a year in these theories.

13
Proton Decay
dr
dr
p0
anti-danti-r
ug
P
Xanti-r
ub
e
14
Particle Spin
  • Orbital angular momentum is quantized to integer
    units of Plancks constant over 2?
  • ? h/2?.
  • Quarks and leptons have half a unit of angular
    momentum as spin, or are spin 1/2 particles, also
    called fermions.
  • Photons and Ws and Z are spin 1 particles, also
    called bosons.
  • Gravitons have spin 2, and are bosons.

15
Particle Supersymmetry
  • In a Grand Unified Theory, all quarks and leptons
    are in a generation are united into one family.
  • The GUT gauge bosons transform one quark or
    lepton to another, such a gluon changing one
    color quark into another.
  • A grander symmetry would be to transform all
    gauge bosons to fermions with the same charges,
    and vice versa.
  • Thus for every spin ½ fermion there would be a
    spin 0 boson with the same charges and flavor,
    and to every gauge boson, there would be a like
    charged and coupled spin ½ fermion.
  • These look-alikes, except for spin, are called
    sparticles.

16
Conserved Supersymmetry
  • If supersymmetryness is conserved, sparticles can
    only be created or destroyed in pairs
  • Sparticles would then decay to the ordinary
    particles plus another sparticle,
  • until they reach the lightest supersymmetric
    particle (LSP)
  • The LSP should be neutral and is a leading dark
    matter candidate
  • They should have masses about 1 TeV
  • They should be produced in pairs at the LHC in
    2007
  • The Next Linear Collider (NLC) will be needed to
    map out the sparticles and Higgs interactions in
    detail.

17
Sparticle Names
  • Thus with quarks there would be spin 0 squarks
  • Leptons would have spin 0 sleptons (selectron and
    sneutrino)
  • The photon also would have a spin ½ photino
  • The Ws and Zs would have spin ½ Winos and Zinos
    (after Wess and Zumino)
  • Spin 0 Higgs would have spin ½ Higgsinos
  • In a supergravity theory, spin 2 gravitons have
    spin 3/2 gravitino look-alikes.

18
Why Supersymmetry (SUSY)?
  • Its believers think it is a beautiful symmetry
    between fermions and bosons, and should be a part
    of nature.
  • If the sparticles are at about 1 TeV, then the
    running coupling constants actually do meet at a
    GUT scale of 1017 GeV.
  • GUT scale (mass) Higgss would normally couple to
    the light SM Higgs and bring its mass up to the
    GUT scale.
  • Adding sparticles to particles cancel this
    coupling to leave the SM Higgs light, solving the
    so-called Heirarchy problem.
  • String Theory requires SUSY, again for similar
    cancellations.

19
Minimal SUSY Standard Model
  • The MSSM has two Higgs doublets, as opposed to
    the one in the standard model.
  • The doublets also have distinct anti-Higgs.
  • Thus there are 8 Higgs particles.
  • Three are eaten to make the W and Z massive.
  • One makes the neutral mass generating Higgs.
  • Four more are observable, of which two are
    charged.

20
Evolution of Gauge Couplings (reciprocals)
Standard Model
Supersymmetry
21
Meeting of the Running Couplings (reciprocals) in
MSSM
22
What is String Theory?
  • It is the theory that elementary particles are
    really strings with tension, that obey relativity
    and quantum mechanics.
  • By dispersing the particle away from a point, it
    avoids infinities in the treatment of gravity or
    gravitons by pointlike particles.
  • The string size is close to the Planck size of
    10-32 cm, which is the smallest size where
    gravity becomes strong.
  • To avoid anomaly infinities requires
    supersymmetry and 10 dimensions (1 time and 9
    space dimensions).
  • String theory then provides a quantum theory of
    gravity.
  • Andre Neveu, John Schwarz, Michael Green and
    Pierre Ramond were founders.

23
Pictures of John Schwarz and Ed Witten
24
Types of Superstring Theories
  • There are five superstring theories.
  • There is one open superstring theory with left
    (L) moving waves (SO(32)).
  • There are two closed superstring theories
  • Type IIA L-R parity symmetric
  • Type IIB L only, parity violating
  • There are two heterotic string theories of a
    product of a string theory in 26 dim (with L
    moving waves) x a superstring in 10 dim (with R
    moving waves).
  • (SO(32)) and (E8 x E8).

25
Unification of Superstring Theories
  • Recently, in the second string revolution, it was
    discovered that there are transformations between
    all five superstring theories. (Ed Witten)
  • This means they are all views of a larger theory
    which is not well understood, but is called M
    theory. It may be in 11 dimensions.
  • For further information, see
  • http//superstringtheory.com/, run by
    Patricia Schwarz, John Schwarzs wife.
  • The Elegant Universe by Brian Greene,
  • http//www.pbs.org/wgbh/nova/elegant

26
Towards Verification of Superstring Theory
  • Since superstring theory included the three
    unified forces of GUTS and gravity, it has been
    called the Theory of Everything.
  • It has not been possible to solve superstring
    theory to find a unique physical model.
  • There are a half-million ways to topologically
    compactify the extra six dimensions to very
    short distances, and leave the four dimensional
    world that we live in.
  • So many GUTS and breakup paths of GUTS to the SM
    are still possible

27
Verification of Superstring Theory
  • The masses of sparticles are not well predicted.
  • If they are in the TeV range, they will appear in
    the LHC.
  • Once they are found, the NLC e e- collider will
    more precisely determine their properties.
  • The convergence of the running coupling strengths
    at a GUT scale is more successful with SUSY
    particles than in the SM.
  • If SUSY is found, it will be considered a success
    of string theory. If not found, it could spell
    its demise.
  • The lightest neutral SUSY particle (LSP) could be
    dark matter, and there are experiments to
    directly detect them, but they will take a while
    to reach large enough scale.

28
How do strings scatter?
  • Via the pants diagram, where two strings merge
    to one, and then go back to two.

29
Speculative Models of Extra Dimensions
  • Large Extra Dimensions and Branes
  • Early Unification with a Strong Gravity

30
Brane Solutions
  • String Theories have membrane solutions
  • The most used is that all our 4 dimensional world
    is a membrane in the 10 dimensional world.
  • Open string ends are attached to the membrane.
  • Quarks, leptons and interacting bosons for strong
    and electroweak particles are confined to the
    brane.
  • But gravitons as closed strings can leave the
    brane and spread out in the extra dimensions.

31
Brane with attached stringand graviton in extra
dimension
32
Large Extra Dimension Models
  • By experimental limits, extra dimensions could
    still be as large as 0.1 millimeter, and this
    will be tested by gravity, which behaves as F
    M1 M2/ rn2 for n extra dimensions, at r lt R.
  • In these, gravity could become strong at 1 TeV
    and unify with the other forces there. (Nima
    Arkani-Hamed, Dimopoulos and Dvali)
  • The extra dimension could be curled up with 1 TeV
    excitations, or at the String or Planck Scale.
  • The former would show up in experiment at
    Fermilab or the LHC as invisible missing energy
    disappearing into the extra dimensions in
    excitations there, or as one micro black hole a
    second being produced.

33
Plane Extra Dimension
  • The extra dimension could be between two flat
    branes, one of which is physical, and one of
    which has gravity (unphysical brane).
  • The gravity field exponentially decreases from
    the unphysical to the physical brane.
  • Thus gravity appears weak to us on the physical
    brane, but is strong on the unphysical brane.
  • Called the Randall-Sundrum model.
  • The extra dimension models so far do not give GUT
    theories, spoiling the supersymmetry triumph of
    explaining the convergence of coupling constants
    at the GUT scale.

34
Relevance of Particle Physics
  • We are closer to accounting for some leftover
    matter, possibly requiring three generations of
    quarks and leptons.
  • We may someday account for inflation and dark
    matter (SUSY?) and dark energy.
  • We understand how the Sun shines through weak
    interactions.
  • We understand how color forces and quarks form
    nucleons.
  • We may soon find how a Higgs gives mass to
    everything.
  • There may be Grand Unification to keep charges of
    everything the same and allow particle changing
    interactions.
  • We may have found a way to have gravity that is
    consistent with quantum mechanics.
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