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One may also add boundaries or defects to the models so far described
in infinite space and exploit the integrability (factorizability) in a similar
fashion as explained in the previous sections. How to treat boundaries
in statistical mechanics, that is how to extend the Yang-Baxter equations,
is known since about twenty years [36
]. Ten years ago we undertook the first attempt to extend these ideas
to QFT [66
] by formulating the bootstrap principle for systems with reflecting
boundaries. We solved the proposed equations for a particular class of
ATFTs [ 67
] and also allowed the boundary to have degrees of freedom [
68
]. Since then an entire industry has developed working according to the
principle: to each bulk theory one can add a boundary and solve it. Of course
it is interesting to have more and more solutions and essentially everything
said in (vi) carries over to this situation. Concerning the general direction
of this activities, there are motivations from string theory (an open string
has naturally a boundary), but I am not aware of concrete investigations
and results in this direction. With regard to applications in condensed
matter physics the situation is different, boundaries are interesting (quantum
wires are finite see (viii)), but possible more relevant are defects and
impurities. One can then treat impurities according to the same factorization
principles of IQFT and introduce besides a reflection also a transmission
amplitude. It is clear that the most interesting situation will be one in
which both types of amplitudes are simultaneously non-vanishing. We showed,
however, [33
] that even in the most general set up with degrees of freedom in the
boundaries this is only possible for theories whose bulk theory is free,
possibly obeying some exotic statistics. In [
25
,26
] we constructed various solutions for simultaneously non-vanishing reflection
and transmission amplitudes for a variety of single multiple defect systems.
In particular the solutions of double defects were very interesting as they
allow for resonances which resemble the behaviour of unstable particles.
Concerning boundaries one should start organizing the existing
solutions and seek for more generic (Lie algebraic) structures analogue
to what has been said in (vi).
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(applications
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