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STRING THEORY: CHALLENGES AND PROSPECTS John H' Schwarz

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Title: STRING THEORY: CHALLENGES AND PROSPECTS John H' Schwarz


1
STRING THEORY CHALLENGES AND PROSPECTS John
H. Schwarz
  • October 2008

2
  • OUTLINE
  • I. What is string theory?
  • II. Challenges and Prospects

3
I. What is String Theory?
  • String theory arose in the late 1960s in an
    attempt to understand the strong nuclear force.
    This is the force that holds neutrons and protons
    together inside the nucleus.
  • The theory must incorporate relativity and
    quantum mechanics. If the fundamental objects in
    the theory are loops or line segments, called
    strings, rather than point-like particles, it can
    account for features of the strong nuclear force.

4
  • The basic idea is that different motions of
    the string correspond to different types of
    particles. So, string theory has a unique
    fundamental object (namely, the string).
  • The original string theory (1968-69), called
    the bosonic string theory, has several fatal
    shortcomings. A much better one, superstring
    theory (1971), overcomes these problems.

5
BOSONIC STRING THEORY
  • This theory describes bosons but not fermions.
    These are the two basic classes of particles in
    quantum theories.
  • Consistency requires 26 dimensions (25 of them
    are spatial and 1 is time).
  • It has various other mathematical and physical
    shortcomings, but it serves as a good warm-up
    exercise.

6
SUPERSTRING THEORY
  • Another string theory that contains both
    fermions and bosons was introduced in 1971 by
    Ramond, Neveu, and me. It requires 10 dimensions
    (9 1).
  • Its development led to the discovery of
    supersymmetry, a symmetry that relates bosons and
    fermions. Strings with this symmetry are called
    superstrings.

7
UNIFICATION
  • Both string theories contain massless
    particles. One of them has just the right
    properties to be the graviton -- the particle
    responsible for the gravitational force.
  • In 1974 Scherk and I proposed using string
    theory for unification of all forces (including
    gravity).

8
EINSTEINS DREAM
  • A unified theory was Einsteins focus in his
    later years. However, the approach he pursued
    involved trying to combine only electromagnetism
    and gravitation (general relativity).
  • The nuclear forces were not yet understood,
    and Einstein was uneasy with quantum mechanics,
    even though he was one of its founders. So his
    efforts were doomed from the outset.

9
THE SIZE OF STRINGS
  • When strings were supposed to describe
    strongly interacting nuclear particles (hadrons)
    their typical size needed to be
  • L 10-13 cm
  • To describe gravity it needs to be roughly
    equal to the Planck length
  • L hG/c3 1/2 10-33 cm
  • Smaller by 20 orders of magnitude!

10
  • Advantages of String Theory
  • for Unification
  • Quantum corrections to Einsteins theory of
    gravity are infinite in point-particle theories.
    In contrast, string theory gives finite results.
  • The extra spatial dimensions can curl up and
    become very small in a gravity theory, where the
    geometry of space and time is determined by the
    dynamics.

11
FIVE THEORIES

Following various breakthroughs in 1984, we had
five consistent superstring theories Type I,
Type IIA, Type IIB, Heterotic HE and HO Each
of these is unique (without any free parameters)
and requires ten dimensions.
12
DUALITIES
  • String theory has many surprising truths. One
    of them is that different geometries for the
    extra dimensions can be physically equivalent!
    This is called T duality.
  • e.g., a circle of radius R can be equivalent
    to a circle of radius L2/R, where L is the string
    length scale. Two such cases are
  • HE ? HO and IIA ? IIB

13
S DUALITY
  • Another surprising discovery is S duality. It
    relates a theory with an interaction strength g
    to another one with interaction strength g
    1/g. Two examples are
  • I ? HO and IIB ? IIB.
  • Thus, since we know how to compute physical
    quantities when g is very small, we learn how
    these three theories behave when g is very large.

14
  • M-THEORY
  • What happens to the other two theories (IIA
    and HE) when g is large?
  • Answer They grow an 11th dimension of size
    gL. This new dimension is a circle in the IIA
    case and a line interval in the HE case.
  • Taken together with the dualities, this
    implies that the five superstring theories are
    actually different facets of a unique
    underlying theory.

15
Theres just one theory!
Courtesy of John Pierre
16
BRANES
  • In addition to fundamental strings,
    superstring theory predicts the existence of
    objects with p spatial dimensions, called
    p-branes. (The fundamental string is a 1-brane.)
  • The values of p that can occur depend on the
    theory. Since the dimension of space is large (9
    or 10), the allowed values of p can also be
    large. For example, M-theory admits a 2-brane and
    a 5-brane.

17
BRANE WORLDS
  • Certain p-branes are called D-branes. They
    have the property that fundamental strings can
    end on them. One consequence is that quantum
    field theories, like the standard model, can live
    on these D-branes.
  • In this setup elementary particles and all
    forces except gravity are restricted to the
    branes, while gravity acts in all ten dimensions.

18
II. CHALLENGES AND PROSPECTS
19
1. Explain Particle Physics
  • The underlying theory is unique, but its
    equations have very many solutions. One of them
    should describe the microscopic quantum world of
    particle physics.
  • Can we find it? Is it picked out by some
    beautiful principle, or is it just randomly
    chosen by our corner of the Universe?

20
Facts to Explain
  • Four-Dimensional Spacetime
  • Yang--Mills Quantum Field Theory with SU(3) X
    SU(2) X U(1) gauge symmetry.
  • Three families of quarks and leptons.
  • The SU(2) X U(1) symmetry is broken to the
    electromagnetic U(1) symmetry by the Higgs
    mechanism. This gives mass to the quarks and
    leptons.

21
2. Understand the Role of Supersymmetry
  • Supersymmetry, which is an essential feature
    of superstring theory, implies that every
    particle has a superpartner.
  • What are their masses?
  • Is the LSP responsible for dark matter?
  • Can superpartners be made in collisions?
  • How is supersymmetry broken?

22
With Supersymmetry
Courtesy of The Particle Adventure
23
7 7 TeV proton proton collider
24
Detectors
25
3. Cosmology Origin and Evolution of the
Universe
  • Trying to understand the whole Universe raises
    similar sorts of questions. How much of its
    origin, structure, and evolution can be deduced
    from first principles?
  • Superstring cosmology has become a very active
    field of research.

26
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27
4. Understand Empty Space
  • Empty space (or the vacuum) contains a
    mysterious substance called dark energy. It
    accounts for about 70 of the total energy of the
    Universe, and it causes the expansion of the
    Universe to accelerate.
  • The density of this energy is 10(-120), when
    expressed in Planck units. How can we understand
    this number?

28
5. Find a Compelling Formulation of the Theory
  • We do not have a compelling formulation of the
    complete underlying theory. This may require some
    new principle.
  • The existence of space and time is likely to
    be an emergent feature of specific solutions that
    is not built into the underlying theory.

29
Spinoffs
  • Mathematical discoveries
  • Properties of high temperature nuclear matter
  • Condensed matter systems, such as high
    temperature superconductors

30
Conclusions
  • String theory unifies disciplines as well as
    forces and particles.
  • We have been exploring string theory for 40
    years, but there is a long way to go.
  • I find it amazing that we might be able to answer
    such basic questions.
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