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Israel Nuclear Society, Yavne; v. 1 p. 21-23; 1973; Annual meeting of the Israel Nuclear Society; Yavne, Israel; 26 Jun 1973
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Bellissard, Jean; Iochum, Bruno; Lima, Ricardo.
Centre National de la Recherche Scientifique, 13 - Marseille (France). Centre de Physique Theorique1975
Centre National de la Recherche Scientifique, 13 - Marseille (France). Centre de Physique Theorique1975
AbstractAbstract
[en] It is shown that any self-dual cone in a real Hilbert space with finite dimensions is homogeneous if and only if it is facially homogeneous (according to the meaning given by Alain Connes). A spectral theory is developed in these cones, which is analogous to that of self-adjoint operators on a Hilbert space of finite dimension
[fr]
On montre que tout cone autopolaire dans un espace de Hilbert reel de dimension finie est homogene si et seulement si il est facialement homogene au sens d'Alain Connes. On developpe une theorie spectrale dans ces cones analogue a celle des operateurs auto-adjoints sur un espace de Hilbert de dimension finieOriginal Title
Cones autopolaires homogenes et facialement homogenes
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Sep 1975; 7 p
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AbstractAbstract
No abstract available
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Available from http://dx.doi.org/10.1070/RM1998v053n01ABEH000004; Abstract only; Country of input: International Atomic Energy Agency (IAEA)
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Speckbacher, Michael; Balazs, Peter, E-mail: speckbacher@kfs.oeaw.ac.at, E-mail: peter.balazs@oeaw.ac.at2020
AbstractAbstract
[en] This paper considers different facets of the interplay between reproducing kernel Hilbert spaces (RKHS) and stable analysis/synthesis processes: first, we analyze the structure of the reproducing kernel of a RKHS using frames and reproducing pairs. Second, we present a new approach to prove the result that finite redundancy of a continuous frame implies atomic structure of the underlying measure space. Our proof uses the RKHS structure of the range of the analysis operator. This in turn implies that all the attempts to extend the notion of Riesz basis to general measure spaces are fruitless since every such family can be identified with a discrete Riesz basis. Finally, we show how the range of the analysis operators of a reproducing pair can be equipped with a RKHS structure. (paper)
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Available from http://dx.doi.org/10.1088/1751-8121/ab573c; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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Journal of Physics. A, Mathematical and Theoretical (Online); ISSN 1751-8121;
; v. 53(1); [20 p.]

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[en] It was discussed the possibility of introducing a multi-resolution in a Hilbert space which is not necessarily a space of functions. It was investigated which of the classical properties can be translated to this more general framework ant the way in which this can be done. It is commented on the procedure proposed by means of many examples
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Nuovo Cimento. B; ISSN 0369-3554;
; v. 116BS12(3); p. 299-315

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[en] It is shown that as a system which can be characterized by a finite-dimensional Hilbert space is observed more and more frequently, the probability that it will always be found in its initial state tends to one
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Foundations of Physics; v. 6(3); p. 367-369
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Hong, Kyungpyo; Oh, Seungsang; Lee, Ho; Lee, Hwa Jeong, E-mail: cguyhbjm@korea.ac.kr, E-mail: figure8@kaist.ac.kr, E-mail: hjwith@kaist.ac.kr, E-mail: seungsang@korea.ac.kr2014
AbstractAbstract
[en] Lomonaco and Kauffman introduced knot mosaic system to give a definition of quantum knot system. This definition is intended to represent an actual physical quantum system. A knot (m, n)-mosaic is an m×n matrix of mosaic tiles which are T0 through T10 depicted, representing a knot or a link by adjoining properly that is called suitably connected. An interesting question in studying mosaic theory is how many knot (m, n)-mosaics are there. Dm,n denotes the total number of all knot (m, n)-mosaics. This counting is very important because the total number of knot mosaics is indeed the dimension of the Hilbert space of these quantum knot mosaics. In this paper, we find a table of the precise values of Dm,n for 4⩽m⩽n⩽6. Mainly we use a partition matrix argument which turns out to be remarkably efficient to count small knot mosaics. (paper)
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Available from http://dx.doi.org/10.1088/1751-8113/47/43/435201; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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Journal of Physics. A, Mathematical and Theoretical (Online); ISSN 1751-8121;
; v. 47(43); [13 p.]

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Coti Zelati, V.; Li Shujie; Wu Shaoping.
International Centre for Theoretical Physics, Trieste (Italy)1991
International Centre for Theoretical Physics, Trieste (Italy)1991
AbstractAbstract
[en] In this paper we study the existence of periodic solutions for second order Hamiltonian systems -u-bar + Au = ∇V(t,u) when V is T-periodic in t and singular in u. More precisely, we assume V(t,x) → +∞ as x → δΩ, for a given open and bounded set Ω is included in RN. We prove the existence of at least one non trivial T-periodic solution by means of variational techniques. (author). 10 refs
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Aug 1991; 9 p
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[en] The mapping of a straight line in the particle-hole space onto the manifold of Slater determinants is found to induce a trajectory whose curvature is between 1 and √3. This curvature depends on the direction of the line, which renders the particle-hole space anisotropic. There are indications that collective motion induces a large curvature of the path
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Journal de Physique. Lettres; ISSN 0302-072X;
; v. 40(8); p. L.177-L.180

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[en] The authors analyze the abelian and non-abelian anomalous gauge theory through the BRS approach. They construct the positive norm Hilbert space and obtain the physical fields in the abelian case. By the same model, we construct the physical subspace in the non-abelian case for a = 2. Finally, they discuss the physical observables and other related problems
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Modern Physics Letters B; CODEN MPLBE; v. 3(17); p. 1711-1724
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