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SUPERSTRING THEORY: PAST, PRESENT, AND FUTURE John H. Schwarz

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String theory arose in the late 1960s in an attempt to understand ... Juan Maldacena Joe Polchinski Nathan Seiberg. Andrew Strominger Cumrun Vafa Edward Witten ... – PowerPoint PPT presentation

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Title: SUPERSTRING THEORY: PAST, PRESENT, AND FUTURE John H. Schwarz


1
SUPERSTRING THEORY PAST, PRESENT, AND FUTURE
John H. Schwarz
  • PITP Showcase Conference
  • May 13, 2005

2
I. 1968 - 1993
  • 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.
  • A theory based on strings, rather than
    point-like particles, can account for various
    features of the strong nuclear force and the
    strongly interacting particles (hadrons).

3
STRING DYNAMICS
For a point particle the motion makes the
invariant length of the world-line extremal.
For a string the motion makes the invariant area
of the world-sheet extremal.
4
  • The basic idea is that different quantum
    states of the string correspond to the different
    types of particles. So, there is a unique
    fundamental object (namely, the string).

This string theory can be quantized, but this is
consistent only for 26 spacetime dimensions (25
are spatial and 1 is time). The string spectrum
contains bosons only (no fermions). Moreover, one
of these bosons is a tachyon.
5
  • By adding fermionic coordinates to the
    world-sheet, another string theory that contains
    fermions (as well as bosons) was constructed
    in 1971 by Pierre Ramond, André Neveu, and me. It
    requires 10 dimensions.
  • Its development led to supersymmetry, a new
    type of symmetry that relates bosons and
    fermions. Strings with this symmetry are called
    superstrings.

6
  • In addition to the unrealistic
    dimension and the tachyon, the string spectrum
    includes particles that are massless, whereas all
    hadrons have positive mass.
  • In the early 1970s a better theory of the
    strong nuclear force, called quantum
    chromodynamics (or QCD), was developed. As a
    result, string theory fell out of favor.

7
  • UNIFICATION
  • One of the massless particles has precisely
    the right properties to be the graviton -- the
    particle responsible for the gravitational force.
  • In 1974 Joël Scherk and I proposed to use
    string theory for the unification of all forces
    (including gravity), rather than just the strong
    nuclear force. Thus we stumbled upon a possible
    realization of Einstein's dream.

8
THE SIZE OF STRINGS
  • When strings were supposed to describe 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!

9
This proposal had two big benefits
  • All prior attempts to describe quantum
    corrections to Einsteins theory of gravity
    assumed point particles. They gave nonsensical
    infinite results (nonrenormalizable ultraviolet
    divergences). String theory is UV finite.
  • Extra spatial dimensions can be compact in
    string theory, where the geometry is determined
    by the dynamics.

10
FIRST SUPERSTRING REVOLUTION
  • In 1984 Michael Green and I discovered that
    superstring theory is free from certain expected
    quantum inconsistencies, called anomalies, for
    two special choices of the symmetry group
  • SO(32) and E8 x E8
  • This raised hopes that a realistic theory can
    be determined just by mathematical consistency.
    The known symmetries fit nicely inside E8 .

11
MBG and JHS Aspen 1984
12
FIVE THEORIES
  • Subsequently, two new superstring theories
    with exactly these symmetries were constructed by
    the Princeton string quartet.

By the time the dust settled, there seemed to be
five consistent superstring theories I, IIA,
IIB, HE, HO each of which requires ten
dimensions.
13
Calabi-Yau Compactification
  • Certain six-dimensional manifolds, called
    Calabi-Yau spaces, solve the equations and give a
    supersymmetric field theory in the remaining four
    dimensions.
  • If one starts with the HE theory, and chooses
    the right CY space, it is possible to come quite
    close to achieving a realistic supersymmetric
    extension of the Standard Model.

14
  • SPACE (or T) DUALITY
  • It was discovered in the late 1980s that
    different geometries for the extra dimensions can
    be physically equivalent!
  • For example, 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

15
II. 1994 - PRESENT
  • The period of discovery in the mid-1990s is
    referred to as the
  • Second Superstring Revolution
  • Some of the most important contributors are
    pictured on the next slide

16
Juan Maldacena Joe Polchinski
Nathan Seiberg
Andrew Strominger Cumrun Vafa
Edward Witten
17
  • STRENGTH (or S) DUALITY
  • This is another duality that relates a theory
    with interaction strength g to one with strength
    1/g.
  • Two examples are
  • I ? HO and IIB ? IIB.
  • Thus, since we know how to do calculations
    when g is very small, we learn how these three
    theories behave when g is very large.

18
  • M THEORY
  • What happens to the other two superstring
    theories IIA and HE when g is large?
  • Answer They grow an eleventh 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.

19
Theres just one theory!
Courtesy of John Pierre
20
BRANES
  • In addition to fundamental strings,
    superstring theory predicts the existence of new
    objects, called p-branes.
  • p is the number of spatial dimensions they
    occupy. (For example, the fundamental string is a
    1-brane.)
  • Since the dimension of space is large (9 or
    10), the allowed values of p can also be large.

21
BRANE WORLDS
  • Certain p-branes are called D-branes. They
    have the property that strings can end on them.
    One consequence is that quantum field theories
    like the standard model can live on D-branes.
  • One intriguing possibility is that the
    observable Universe is actually a set of
    3-branes, which is embedded in a space with 6
    additional spatial dimensions.

22
ADS/CFT DUALITY
  • In 1997 Maldacena proposed a new
    class of dualities (or equivalences) for
    example, between a certain 4d QFT called N 4
    super Yang-Mills theory and Type IIB superstring
    theory in the 10d geometry AdS5 X S5.
  • The string theory is represented
    holographically by the QFT, which is associated
    to the conformal boundary of the 10d or 11d
    spacetime. Since the QFT is conformally invariant
    (CFT), this is called an AdS/CFT duality.

23
III. SOME REMAINING PROBLEMS
  • 1. Find a complete and compelling formulation of
    the theory
  • We do not yet have a compelling
    formulation of the underlying theory. It may
    require some principle that has not yet been
    understood.
  • The existence of space and time is probably
    an emergent feature of specific solutions that is
    not built into the underlying theory.

24
  • 2. Understand empty space
  • The vacuum energy density, called dark energy,
    is observed to be about 70 of the total energy
    of the present Universe. It causes the expansion
    of the Universe to accelerate.
  • This energy density is only about 10-122 when
    expressed in Planck units. Anthropic explanation
    If it were much larger, we wouldnt be here. Is
    there another explanation? I hope so.

25
3. Explain elementary particle physics
  • Superstring theory may be unique, but its
    equations have very many solutions (or quantum
    vacua). 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?

26
4. Understand the role of supersymmetry
  • Supersymmetry requires that every particle
    have a superpartner.
  • What are their masses?
  • Is the lightest superpartner (LSP) responsible
    for dark matter?
  • Can superpartners be made in collisions?

27
With Supersymmetry
Courtesy of The Particle Adventure
28
5. Understand spacetime and quantum mechanics
  • What prevents bad spacetime singularities?
  • What ensures causality?
  • What are the microscopic quantum states that
    are responsible for the entropy of black holes?
  • Is quantum mechanics exact?
  • What ensures that there is no loss of quantum
    coherence for processes involving black holes?

29
Trying to understand the whole Universe raises
yet more questions. How much of its origin,
structure, and evolution can be deduced from
first principles?
6. Understand the origin and evolution of the
Universe
Observational cosmology is providing many facts
that need to be explained. Superstring cosmology
has recently become a very active field of
research.
30
7. Develop mathematical techniques and concepts
  • String theory is up against the frontiers of
    several branches of mathematics. Given our
    experience to date, I expect that future
    developments will require mathematical methods
    and concepts that do not currently exist.
  • String theory is unifying disciplines as well
    as forces and particles.
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