By Swanhild Bernstein, Uwe Kähler, Irene Sabadini, Frank Sommen

ISBN-10: 3319087703

ISBN-13: 9783319087702

ISBN-10: 3319087711

ISBN-13: 9783319087719

Hypercomplex research is the extension of complicated research to better dimensions the place the idea that of a holomorphic functionality is substituted by means of the concept that of a monogenic functionality. In contemporary many years this idea has come to the vanguard of upper dimensional research. There are a number of methods to this: quaternionic research which in basic terms makes use of quaternions, Clifford research which will depend on Clifford algebras, and generalizations of complicated variables to raised dimensions equivalent to split-complex variables. This publication contains a collection of papers awarded on the consultation on quaternionic and hypercomplex research on the ISAAC convention 2013 in Krakow, Poland. the themes coated symbolize new views and present tendencies in hypercomplex research and purposes to mathematical physics, photo research and processing, and mechanics.

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Hypercomplex research is the extension of complicated research to raised dimensions the place the idea that of a holomorphic functionality is substituted by means of the idea that of a monogenic functionality. In contemporary a long time this conception has come to the vanguard of upper dimensional research. There are a number of ways to this: quaternionic research which in basic terms makes use of quaternions, Clifford research which depends on Clifford algebras, and generalizations of advanced variables to raised dimensions resembling split-complex variables.

**Extra info for Hypercomplex Analysis: New Perspectives and Applications**

**Sample text**

This equality is true on Ω ∩ R+ , and extends to Ω by where b(p) = 1+px 0 slice hyperholomorphic extension. 2, we now assume 0 ∈ Ω. 5) be a coisometric realization of S. Then A has a unique maximal strictly negative invariant subspace M. 7. 3. The rest of the proof is as in [9], and is as follows. Let M be the space deﬁned in STEP 2, and let AM , CM denote the matrix representations of A and 36 D. Alpay, F. Colombo and I. Sabadini C, respectively, in a basis of M, and let GM be the corresponding Gram matrix.

In the treatment in [22] no tensor products of Hilbert-Cliﬀord modules are involved. In the framework of slice hyperholomorphic analysis we have already introduced and studied the Hardy spaces (see [7, 3, 4]), and Bergman spaces (see [18, 20, 19]). Here we begin the study of the main properties of the quaternionic Fock spaces. We start by recalling the deﬁnition of the Fock space in the classical complex analysis case (for the origins of the theory see [24]). For n ∈ N let z = (z1 , . . , zn ) ∈ Cn where zj = xj + iyj , xj , yj ∈ R (j = 1, .

Birkh¨ auser, 2001. [20] A. Bloch. Les fonctions holomorphes et m´eromorphes dans le cercle unit´e. M´emorial des sciences math´ematiques, pages 1–61, 1926. Fascicule 20. [21] J. Bogn´ ar. Indeﬁnite inner product spaces. Ergebnisse der Mathematik und ihrer Grenzgebiete, Band 78. Springer-Verlag, Berlin, 1974. 40 D. Alpay, F. Colombo and I. Sabadini [22] V. Bolotnikov and L. Rodman. Krein–Langer factorizations via pole triples. Integral Equations and Operator Theory, 47(2):169–195, 2003. [23] C.

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