On the Cauchy theorem for hyperholomorphic functions of spatial variable

We proved a theorem about the integral of quaternionic-differentiable functions of spatial variable over the closed surface. It is an analog of the Cauchy theorem from complex analysis.

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Дата:2017
Автор: Herus, O.F.
Формат: Стаття
Мова:English
Опубліковано: Інститут прикладної математики і механіки НАН України 2017
Назва видання:Український математичний вісник
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/169319
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Цитувати:On the Cauchy theorem for hyperholomorphic functions of spatial variable / O.F. Herus // Український математичний вісник. — 2017. — Т. 14, № 2. — С. 153-160. — Бібліогр.: 15 назв. — англ.

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spelling irk-123456789-1693192020-06-11T01:26:28Z On the Cauchy theorem for hyperholomorphic functions of spatial variable Herus, O.F. We proved a theorem about the integral of quaternionic-differentiable functions of spatial variable over the closed surface. It is an analog of the Cauchy theorem from complex analysis. 2017 Article On the Cauchy theorem for hyperholomorphic functions of spatial variable / O.F. Herus // Український математичний вісник. — 2017. — Т. 14, № 2. — С. 153-160. — Бібліогр.: 15 назв. — англ. 1810-3200 2010 MSC. 30G35, 32V05 http://dspace.nbuv.gov.ua/handle/123456789/169319 en Український математичний вісник Інститут прикладної математики і механіки НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
description We proved a theorem about the integral of quaternionic-differentiable functions of spatial variable over the closed surface. It is an analog of the Cauchy theorem from complex analysis.
format Article
author Herus, O.F.
spellingShingle Herus, O.F.
On the Cauchy theorem for hyperholomorphic functions of spatial variable
Український математичний вісник
author_facet Herus, O.F.
author_sort Herus, O.F.
title On the Cauchy theorem for hyperholomorphic functions of spatial variable
title_short On the Cauchy theorem for hyperholomorphic functions of spatial variable
title_full On the Cauchy theorem for hyperholomorphic functions of spatial variable
title_fullStr On the Cauchy theorem for hyperholomorphic functions of spatial variable
title_full_unstemmed On the Cauchy theorem for hyperholomorphic functions of spatial variable
title_sort on the cauchy theorem for hyperholomorphic functions of spatial variable
publisher Інститут прикладної математики і механіки НАН України
publishDate 2017
url http://dspace.nbuv.gov.ua/handle/123456789/169319
citation_txt On the Cauchy theorem for hyperholomorphic functions of spatial variable / O.F. Herus // Український математичний вісник. — 2017. — Т. 14, № 2. — С. 153-160. — Бібліогр.: 15 назв. — англ.
series Український математичний вісник
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fulltext Український математичний вiсник Том 14 (2017), № 2, 153 – 160 On the Cauchy theorem for hyperholomorphic functions of spatial variable Oleg F. Herus (Presented by V. Ya. Gutlyanskii) Abstract. We proved a theorem about integral of quaternionic- differentiable functions of spatial variable over the closed surface. It is an analog of the Cauchy theorem from complex analysis. 2010 MSC. 30G35, 32V05. Key words and phrases. Quaternion, Dirac operator, differentiable function. 1. Introduction Several researchers (see, e.g., [1, 2]) tried to generalize methods of complex analysis onto analysis of functions acting in several-dimensional algebras. At that, generalizations of different but mutually equivalent definitions of holomorphy in complex analysis generate diverse classes of hyperholomorphic functions in several-dimensional algebras. Hypercomplex analysis in the space R3 was launched in the work of G. Moisil and N. Theodoresco [3], where a three-dimensional analog of the Cauchy–Riemann system was posed for the first time. R. Fueter [4] first introduced a class of “regular” quaternion functions by means of a four-dimensional generalization of the G. Moisil and N. Theodoresco system. He proved quaternion analogues of the Cauchy theorem, the integral Cauchy formula, the Liouville theorem and constructed an analog of the Laurent series. Now quaternion analysis gained wide evolution (more detailed see [1, 5–7]) previously thanks to its physical applications. At that in most works it was usual to consider functions having continuous partial derivatives in a domain and satisfying the above Cauchy–Riemann-type system. In particular in the book [1] a spatial analog of the Cauchy theorem was Received 20.03.2017 ISSN 1810 – 3200. c⃝ Iнститут прикладної математики i механiки НАН України 154 On the Cauchy theorem for hyperholomorphic... proved by using the quaternion Stokes formula for bounded domains with a piecewise-smooth boundary and for functions having continuous partial derivatives in the closure of the domain. In the survey paper [6] the continuity of partial derivatives was re- placed by the weaker condition of real-differentiability for components of the quaternion function. In the work [8] we consider the same class of functions defined in a three-dimensional domain with the piecewise- smooth boundary and requiring only the component-wise real-differenti- ability and satisfying Cauchy–Riemann-type conditions like the class of holomorphic functions in complex analysis (see e.g. [9]). In the present work we extend the result of the paper [8] onto more wide class of surfaces by using methods of the work [10], where a simi- lar theorem was proved for functions taking values in finite-dimensional commutative associative algebras. 2. Quaternion hyperholomorphic functions Let H(C) be the associative algebra of complex quaternions a = 3∑ k=0 akik, where {ak}3k=0 ⊂ C, i0 = 1 and i1, i2, i3 be the imaginary quaternion units with the multiplication rule i21 = i22 = i23 = i1i2i3 = −1. The module of quaternion is defined by the formula |a| := √√√√ 3∑ k=0 |ak|2. Lemma 2.1 ( [11]). |ab| 6 √ 2 |a| |b| for all {a; b} ⊂ H(C). For {zk}3k=1 ⊂ R consider vector quaternions z := z1i1 + z2i2 + z3i3 as points of the Euclidean space R3 with the basis {ik}3k=1. Let Ω be a domain of R3. For functions f : Ω → H(C) having first order partial derivatives consider differential operators Dl[f ] := 3∑ k=1 ik ∂f ∂zk , Dr[f ] := 3∑ k=1 ∂f ∂zk ik. O. F. Herus 155 Definition 2.1. Function f := f0 + f1i1 + f2i2 + f3i3 is called left- or right-H-differentiable in a point z(0) ∈ R3 if its components f0, f1, f2, f3 are R3-differentiable functions in z(0) and the next condition Dl[f ](z (0)) = 0 (2.1) or Dr[f ](z (0)) = 0 holds true respectively. There is the notion of C-differentiability of a function f(ζ) = u(x, y)+ v(x, y)i, ζ = x+yi, in complex analysis (see [9, p. 33–34]). It is equivalent to R2-differentiability in the point (x0, y0) of the components u(x, y) and v(x, y) and satisfaction the condition ∂f(ζ0) ∂x + ∂f(ζ0) ∂y i = 0. Thus the defined above notion of H-differentiability is the exact analog of C-differentiability from complex analysis. It is well known (see [9, p. 35]) that C-differentiability of a complex function is equivalent to existence of its derivative. But in quaternion analysis only the linear functions of special form have a derivative (see [12]). The operator Dl is called the Dirac operator (see [13]) or the Moisil– Theodoresco operator (see [14]) and equality (2.1) is equivalent to the Moisil–Theodoresco system [3]. Definition 2.2. A function f is called left- or right-hyperholomorphic in a domain Ω if it is left- or right-H-differentiable in every point of the domain. 3. Quaternion surface integral Consider notions of surface and closed surface like to defined in the work [10]. Definition 3.1. A surface Γ ⊂ R3 is an image of a closed set G ⊂ R2 under a homeomorphic mapping φ : G→ R3 φ(u, v) := (z1(u, v), z2(u, v), z3(u, v)), (u, v) ∈ G, such that Jacobians A := ∂z2 ∂u ∂z3 ∂v −∂z2 ∂v ∂z3 ∂u , B := ∂z3 ∂u ∂z1 ∂v −∂z3 ∂v ∂z1 ∂u , C := ∂z1 ∂u ∂z2 ∂v −∂z1 ∂v ∂z2 ∂u exist almost everywhere on the set G and summable on G. 156 On the Cauchy theorem for hyperholomorphic... The area of the surface Γ is calculated by the formula L(Γ) = ∫∫ G √ A2 +B2 + C2dudv, where the integral is understood in the Lebesgue sense. A surface Γ is called quadrable (see [10]) if L(Γ) < +∞. Let Γ ⊂ R3 be an image of a sphere S ⊂ R3 in a such homeomorphic mapping ψ : S → R3 that the image of a great circle γ on the sphere S is a closed Jordan rectifiable curve γ̃ on the set Γ. The sphere S is the union of two half-spheres S1, S2 with common edge γ. It is ease to see that there exist continuously differentiable mappings φ1 : K → S1, φ2 : K → S2 of the disk K := {(u, v) ∈ R2 : u2 + v2 6 1}. So the set Γ is the union of two sets Γ1 = ψ(φ1(K)), Γ2 = ψ(φ2(K)) with the intersection γ̃ = ψ(φ1(∂K)) = ψ(φ2(∂K)). Definition 3.2. A set Γ is called a closed surface if there exist a such homeomorphic mapping ψ : S → R3 that the sets Γ1, Γ2 are surfaces in the sense of Definition 3.1 and orientation of the circle ∂K induces two mutually opposite orientations of the curve γ̃ under mappings ψ ◦φ1 and ψ ◦ φ2 respectively. Let Γε := { z ∈ R3 : ρ(z,Γ) 6 ε } (ρ denotes the Euclidean distance) be the closed ε-neighborhood of the surface Γ, V (Γε) be the space Lebes- gue measure of the set Γε and M∗(Γ) := lim ε→0 V (Γε) 2ε be the two-dimensional upper Minkowski content (see [15, p. 79]) of the surface Γ. For functions f : Γ → H(C), g : Γ → H(C) in the case of non-closed quadrable surface Γ the quaternion surface integral is defined by the formula∫∫ Γ f(z)σ g(z) := ∫∫ G f(φ(u, v))(Ai1 +Bi2 + Ci3)g(φ(u, v))du dv, where σ := dz2dz3i1 + dz3dz1i2 + dz1dz2i3, and in the case of a closed surface — by the formula∫∫ Γ f(z)σ g(z) := ∫∫ Γ1 f(z)σ g(z) + ∫∫ Γ2 f(z)σ g(z). In particular, ∫∫ Γ |σ| = L(Γ). Theorem 3.1 ( [8]). Let P be the surface of a closed cube contained in a simply connected domain Ω ⊂ R3, let a function f : Ω → H(C) be right- hyperholomorphic and a function g : Ω → H(C) be left-hyperholomorphic. O. F. Herus 157 Then ∫∫ P f(z)σ g(z) = 0. Let δ > 0, let ωΓ(f, δ) := sup |z1−z2|6δ z1,z2 ∈Γ |f(z1)− f(z2)| be the module of continuity of a function f on Γ, and let d(Γ) be the diameter of Γ. Lemma 3.1 ( [10]). Let Γ be a quadrable closed surface. Then∫∫ Γ σ = 0. (3.1) Lemma 3.2. Let Γ be a quadrable closed surface and let f : Ω → H(C) and g : Ω → H(C) be continuous functions. Then∣∣∣∣∣∣ ∫∫ Γ f(z)σ g(z) ∣∣∣∣∣∣ 6 2L(Γ) ( ωΓ(f, d(Γ)) max z∈Γ |g(z)|+ ωΓ(g, d(Γ)) max z∈Γ |f(z)| ) . (3.2) Proof. Thanks to the formula (3.1) we have∫∫ Γ f(z0)σ g(z0) = 0 for any point z0 ∈ Γ. Therefore∫∫ Γ f(z)σ g(z) = ∫∫ Γ (f(z)− f(z0))σ g(z0) + ∫∫ Γ f(z)σ (g(z)− g(z0)), from which follows the estimate (3.2), taking into account Lemma 2.1. Theorem 3.2. Let R3 ⊃ Ω be a bounded simply connected domain with the quadrable closed boundary Γ, for which M∗(Γ) < +∞, (3.3) 158 On the Cauchy theorem for hyperholomorphic... let Ω have Jordan measurable intersections with planes perpendicular to coordinate axes, let a function f : Ω → H(C) be right-hyperholomorphic in Ω and continuous in the closure Ω and let a function g : Ω → H(C) be left-hyperholomorphic in Ω and continuous in Ω. Then∫∫ Γ f(z)σ g(z) = 0. (3.4) Proof. Let us use the method proposed in the work [10] under the prov- ing of Theorem 6.1. Thanks to the condition (3.3) there exists such a constant c > 0 that for all sufficiently small ε > 0 the following inequality holds V (Γε) 6 cε. (3.5) Decompose the space by planes perpendicular to coordinate axes onto closed cubes with the edge of length ε√ 3 . Let {Kj}, j ∈ J , be the finite set of formed cubes having nonempty intersection with the surface Γ. The integral (3.4) is representable in the form∫∫ Γ f(z)σ g(z) = ∑ j∈J ∫∫ ∂(Ω∩Kj) f(z)σ g(z) + ∑ Kj⊂Ω ∫∫ ∂Kj f(z)σ g(z). (3.6) By the Theorem 3.1 the second sum in the equality (3.6) is equal zero. Every set Ω ∩ Kj consists of finite or infinite totality of connected components. Applying the estimate (3.2) to the boundary of the every component, we obtain∣∣∣∣∣∣∣ ∫∫ ∂(Ω∩Kj) f(z)σ g(z) ∣∣∣∣∣∣∣ 6 2(L(Γ ∩Kj) + 2ε2) ( ωΓ(f, ε) max z∈Ω |g(z)| + ωΓ(g, ε) max z∈Ω |f(z)| ) . (3.7) Substituting the inequality (3.7) into the equality (3.6), we obtain∣∣∣∣∣∣ ∫∫ Γ f(z)σ g(z) ∣∣∣∣∣∣ 6 2 L(Γ) + 2 ∑ j∈J ε2 (ωΓ(f, ε) max z∈Ω |g(z)|+ ωΓ(g, ε) max z∈Ω |f(z)| ) . O. F. Herus 159 Since ∪ j∈J Kj ⊂ Γε, we obtain from the inequality (3.5) that 1 3 √ 3 ∑ j∈J ε3 6 V (Γε) 6 cε. Therefore∣∣∣∣∣∣ ∫∫ Γ f(z)σ g(z) ∣∣∣∣∣∣ 6 2(L(Γ) + 6 √ 3c) ( ωΓ(f, ε) max z∈Ω |g(z)|+ ωΓ(g, ε) max z∈Ω |f(z)| ) and the equality (3.4) be obtained from here by passaging to the limit when ε→ 0. References [1] V. V. Kravchenko, M. V. Shapiro, Integral representations for spatial models of mathematical physics, Addison Wesley Longman, Pitman Research Notes in Mathematics Series, 351, 1996. [2] F. Brackx, R. Delanghe, F. Sommen, Clifford Analysis, Addison Wesley Longman. Pitman Research Notes in Mathematics, 76, 1982. [3] G. C. Moisil, N. Theodoresco, Functions holomorphes dans l’espace // Mathe- matica (Cluj), 5 (1931), 142–159. [4] R. Fueter, Die Funktionentheorie der Differentialgleichungen ∆u = 0 und ∆∆u = 0 mit vier reellen Variablen // Comment. Math. Helv., 8 (1936), 371–378. [5] K. Gürlebeck, W. Sprössig, Quaternionic and Clifford Calculus for Physicists and Engineers, John Wiley & Sons, 1997. [6] A. Sudbery, Quaternionic Analysis // Math. Proc. Camb. Phil. Soc., 85 (1979), 199–225. [7] V. V. Kravchenko, Applied quaternionic analysis, Heldermann-Verlag, Research and Exposition in Mathematics Series, 28, 2003. [8] O. F. Herus On hyperholomorphic functions of the space variable // Ukr. Mat. Zh, 63, (2011), No. 4, 459–465. [9] B. V. Shabat, Introduction to complex analysis. Part 1. Functions of one variable, Moscow, Nauka, 1976 [in Russian]. [10] S. A. Plaksa, V. S. Shpakivskyi, Cauchy theorem for a surface integral in commu- tative algebras // Complex Variables and Elliptic Equations, 59 (2014), No. 1, 110–119. [11] O. F. Gerus, M. V. Shapiro, On a Cauchy-type integral related to the Helmholtz operator in the plane // Boletin de la Sociedad Matemática Mexicana, 10 (2004), N 1, 63–82. [12] A. S. Meilikhzon, On the monogenity of quaternions // Doklady Akad. Nauk SSSR, 59 (1948), No. 3, 431–434. 160 On the Cauchy theorem for hyperholomorphic... [13] J. Cnops, An introduction to Dirac operators on manifolds, Progress in Mathe- matical Physics. 24. Birkhäuser, Boston, 2002. [14] R. A. Blaya, J. B. Reyes, M. Shapiro, On the Laplasian vector fields theory in domains with rectifiable boundary // Mathematical Methods in the Applied Sci- ences, 29 (2006), 1861–1881. [15] P. Mattila, Geometry of sets and measures in Euclidean spaces. Fractals and rectifiability, Cambridge, Cambridge University Press, 1995. Contact information Oleg F. Herus Zhytomyr Ivan Franko State University, Zhytomyr, Ukraine E-Mail: ogerus@zu.edu.ua