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    Polarization Elements-A Group Theoretical Study

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    The Classification of Polarization elements, the polarization affecting optical devices which have a Jones matrix representation, according to the types of eigenvectors they possess, is given a new visit through the Group-theoretical connection of polarization elements. The diattenuators and retarders are recognized as the elements corresponding to boosts and rotations respectively. The structure of homogeneous elements other than diattenuators and retarders are identified by giving the quaternion corresponding to these elements. The set of degenerate polarization elements is identified with the so called `null' elements of the Lorentz Group. Singular polarization elements are examined in their more illustrative Mueller matrix representation and finally the eigenstructure of a special class of singular Mueller matrices is studied.Comment: 7 pages, 2 tables, submitted to `Optics Communications

    Elements of the Continuous Renormalization Group

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    These two lectures cover some of the advances that underpin recent progress in deriving continuum solutions from the exact renormalization group. We concentrate on concepts and on exact non-perturbative statements, but in the process will describe how real non-perturbative calculations can be done, particularly within derivative expansion approximations. An effort has been made to keep the lectures pedagogical and self-contained. Topics covered are the derivation of the flow equations, their equivalence, continuum limits, perturbation theory, truncations, derivative expansions, identification of fixed points and eigenoperators, and the role of reparametrization invariance. Some new material is included, in particular a demonstration of non-perturbative renormalizability, and a discussion of ultraviolet renormalons.Comment: Invited lectures at the Yukawa International Seminar '97. 20 pages including 6 eps figs. LaTeX. PTPTeX style files include

    Computing simplicial representatives of homotopy group elements

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    A central problem of algebraic topology is to understand the homotopy groups πd(X)\pi_d(X) of a topological space XX. For the computational version of the problem, it is well known that there is no algorithm to decide whether the fundamental group π1(X)\pi_1(X) of a given finite simplicial complex XX is trivial. On the other hand, there are several algorithms that, given a finite simplicial complex XX that is simply connected (i.e., with π1(X)\pi_1(X) trivial), compute the higher homotopy group πd(X)\pi_d(X) for any given d2d\geq 2. %The first such algorithm was given by Brown, and more recently, \v{C}adek et al. However, these algorithms come with a caveat: They compute the isomorphism type of πd(X)\pi_d(X), d2d\geq 2 as an \emph{abstract} finitely generated abelian group given by generators and relations, but they work with very implicit representations of the elements of πd(X)\pi_d(X). Converting elements of this abstract group into explicit geometric maps from the dd-dimensional sphere SdS^d to XX has been one of the main unsolved problems in the emerging field of computational homotopy theory. Here we present an algorithm that, given a~simply connected space XX, computes πd(X)\pi_d(X) and represents its elements as simplicial maps from a suitable triangulation of the dd-sphere SdS^d to XX. For fixed dd, the algorithm runs in time exponential in size(X)size(X), the number of simplices of XX. Moreover, we prove that this is optimal: For every fixed d2d\geq 2, we construct a family of simply connected spaces XX such that for any simplicial map representing a generator of πd(X)\pi_d(X), the size of the triangulation of SdS^d on which the map is defined, is exponential in size(X)size(X)

    Group ring elements with large spectral density

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    Given an arbitrary d>0 we construct a group G and a group ring element S in Z[G] such that the spectral measure mu of S has the property that mu((0,eps)) > C/|log(eps)|^(1+d) for small eps. In particular the Novikov-Shubin invariant of any such S is 0. The constructed examples show that the best known upper bounds on mu((0,eps)) are not far from being optimal.Comment: 19 pages, v3: Changes suggested by a referee; Essentially this is the version published in Math. An
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