arXiv:hep-th/9304011 v1 Apr 5 1993
arXiv:hep-th/9304011 v1 Apr 5 1993
arXiv:hep-th/9304011 v1 Apr 5 1993
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Exercise. Missing lessons<br />
Determine which of <strong>th</strong>e lessons below are covered quite elegantly in portions of text<br />
<strong>th</strong>at have been omitted from <strong>th</strong>ese lecture notes [0] but will be restored for <strong>th</strong>e book<br />
version [19].<br />
15.1. Lessons<br />
From <strong>th</strong>e quantum gravity point of view, <strong>th</strong>e main lessons we have learned from <strong>th</strong>e matrix<br />
model are:<br />
• Euclidean Quantum Gravity makes sense, at least in two dimensions.<br />
• The nature of quantum states in Euclidean quantum gravity, and <strong>th</strong>eir interpretation<br />
wi<strong>th</strong>in <strong>th</strong>e quantum mechanical framework is surprising, and requires <strong>th</strong>e introduction<br />
of non-normalizable wavefunctions as well as normalizable wavefunctions.<br />
• The Wheeler–DeWitt constraint is violated in topology-changing processes.<br />
• The contributions of singular geometries to <strong>th</strong>e pa<strong>th</strong> integral of quantum gravity are<br />
important.<br />
• There is a phase of topological gravity which can be connected to phases of nontopological<br />
gravity.<br />
From <strong>th</strong>e string <strong>th</strong>eory point of view, <strong>th</strong>e main lessons we have learned from <strong>th</strong>e matrix<br />
model are:<br />
• Nonperturbative definitions of string physics, at least in some target spaces, exist.<br />
• There are backgrounds wi<strong>th</strong> large unbroken symmetries, e.g., w 1+∞ and volume preserving<br />
diffeomorphism algebras.<br />
• The large order behavior of perturbation <strong>th</strong>eory at order g has <strong>th</strong>e typically “stringy”<br />
(2g)! grow<strong>th</strong>.<br />
• In solvable string <strong>th</strong>eories, <strong>th</strong>ere is a beautiful ma<strong>th</strong>ematical framework (KP flow,<br />
W -constraints, etc.) <strong>th</strong>at relates string physics in different backgrounds.<br />
• Wi<strong>th</strong> current understanding, it is fundamentally impossible to achieve complete background<br />
independence: There is always dependence on boundary and initial conditions<br />
associated wi<strong>th</strong> non-normalizable states.<br />
• There is a phase of string <strong>th</strong>eory which is topological, and can be connected to nontopological<br />
phases wi<strong>th</strong> local physics (such as string scattering in two dimensions).<br />
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