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In [[mathematics]], '''quaternionic analysis''' is the study of functions with [[quaternion]]s as the domain and/or range. Such functions can be called '''functions of a quaternion variable''' just as functions of a [[real variable]] or functions of a [[complex variable]] are called.


As with complex and real analysis, it is possible to study the concepts of [[analytic function|analyticity]], [[holomorphy]], [[harmonic function|harmonicity]] and [[conformality]] in the context of quaternions. It is known that for the complex numbers, these four notions coincide; however, for the quaternions, and also the real numbers, not all of the notions are the same.


==Discussion==
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The [[projection (linear algebra)|projections]] of a quaternion onto its scalar part or onto its vector part, as well as the modulus and [[versor]] functions, are examples that are basic to understanding quaternion structure. An important example of a function of a quaternion variable is
:<math>f(q) = u q u^{-1}</math>
which [[quaternions and spatial rotation|rotates the vector part of ''q'']] by twice the angle of ''u''.
 
The quaternion inversion <math>f(q) = q^{-1}</math> is another fundamental function, but it introduces questions ''f''(0) = ? and "Solve ''f''(''q'') = 0." [[Affine transformation]]s
of quaternions have the form
:<math>f(q) = a q + b, \quad a, b \in \mathbb{H}. </math>
Linear fractional transformations of quaternions can be represented by elements of the [[matrix ring]] M<sub>2</sub>(H) operating on the [[projective line over a ring|projective line over H]]. For instance, the mappings <math>q \mapsto u q v,</math> where {{mvar|u}} and {{mvar|v}} are fixed [[versor]]s serve to produce the [[elliptic geometry#elliptic space|motions of elliptic space]].
 
Quaternion variable theory differs in some respects from complex variable theory as in this instance: The [[complex conjugate]] mapping of the complex plane is a central tool but requires the introduction of a non-arithmetic operation. Indeed, conjugation changes the [[orientation (mathematics)|orientation]] of plane figures, something that arithmetic functions do not change. In contrast, the quaternion conjugation can be expressed arithmetically:
 
'''Proposition:''' The function <math>f(q) = - \tfrac 1 2 (q + iqi + jqj + kqk)</math> is equivalent to quaternion conjugation.
 
Proof: For the basis elements we have
:<math>f(1) = -\tfrac 1 2 (1-1-1-1) = 1, f(i) = -\tfrac 1 2 (i-i+i+i) = -i, f(j) = -j, f(k) = -k </math>.
Consequently, since ''f'' is a [[linear function]],
:<math> f(q) \ = f(w + xi + yj + zk) \ = w f(1) + x f(i) + y f(j) + z f(k) \ = w - x i - y j - zk \ =  q^*.</math>
 
The success of [[complex analysis]] in providing a rich family of [[holomorphic function]]s for scientific work has engaged some workers in efforts to extend the planar theory, based on complex numbers, to a 4-space study with functions of a quaternion variable. These efforts were summarized in 1973 by C.A. Deavours. He recalls a 1935 issue of [[Commentarii Mathematici Helvetici]] where an alternative theory of "regular functions" was initiated by [[Rudolf Fueter|R. Fueter]] through the idea of [[Morera's theorem]]: quaternion function F is "left regular at ''q'' " when the integral of F vanishes over any sufficiently small [[hypersurface]] containing ''q''. Then the analogue of [[Liouville's theorem (complex analysis)|Liouville's theorem]] holds: the only quaternion function regular with bounded norm in E<sup>4</sup> is a constant. One approach to construct regular functions is to use [[power series]] with real coefficients. Deavours also gives analogues for the [[Poisson integral]], the [[Cauchy integral formula]], and the presentation of [[Maxwell’s equations]] of electromagnetism with quaternion functions.
 
Though '''H''' [[quaternion#H as a union of complex planes|appears as a union of complex planes]], the following proposition shows that extending complex functions requires special care:
 
'''Proposition:''' Let <math>f(z) = u(x,y) + i v(x,y)</math> be a function of a complex variable, <math>z = x + i y</math>. Suppose also that ''u'' is an [[even function]]  of ''y'' and that ''v'' is an [[odd function]] of ''y''. Then <math>f(q) = u(x,y) + r \ v(x,y)</math> is an extension of ''f'' to a quaternion variable <math> q = x + y r, \quad r^2 = -1, \quad r \in \mathbb{H} </math>.
 
Proof: Let ''r*'' be the conjugate of ''r'' so that ''q'' = ''x'' &minus; ''y r*''. The extension to '''H''' will be complete when it is shown that ''f(q)'' = ''f(x'' &minus; ''y r*''). Indeed, by hypothesis
:<math>u(x,y)=u(x,-y), \quad v(x,y) = -v(x,-y) \quad</math> so that one obtains
:<math>f(x-yr^*) = u(x,-y) + r^* v(x,-y) = u(x,y) + r \ v(x,y) = f(q).</math>
 
Since the time of Hamilton, it has been realized that requiring the independence of the derivative from the path that a differential follows toward zero is too restrictive: it excludes even <math>f(q) = q^2</math> from differentiability. Therefore a direction-dependent derivative is necessary for functions of a quaternion variable.
 
== The Gâteaux derivative for quaternions ==
The [[Gâteaux derivative]] of a quaternionic function ''f(x)'' is given by
 
:<math>\partial f(x)(h)=\lim_{t\to 0 \in R}(t^{-1}(f(x+th)-f(x)))</math>
 
where ''h'' is a quaternion indicating the direction in which the derivative is to be taken. On the quaternions, the Gateaux derivative will always be [[linear mapping|linear]] in ''h'', so it may be expressed
as
:<math>\partial f(x)(h)= \sum_s \frac{{}_{(s)0}\partial f(x)}{\partial x} h
                        \frac{{}_{(s)1}\partial f(x)}{\partial x}.\,\!
</math>
 
The number of terms in the sum will depend on the function ''f''. The expressions
 
:<math>\frac{{}_{(s)p}\partial f(x)}{\partial x}, \ p=0,1\,\!</math>
 
are called components of the Gateaux derivative.
 
For the function ''f''(''x'') = ''axb'', the derivative is
 
:<math>\partial f(x)(h)=ahb\,\!</math>
 
and so the components are:
{| class="wikitable"
|-
| <math>\frac{{}_{(1)0}\partial axb}{\partial x}=a\,\!</math>
| <math>\frac{{}_{(1)1}\partial axb}{\partial x}=b\,\!</math>
|}
 
Similarly, for the function ''f''(''x'') = ''x''<sup>2</sup>, the derivative is
 
:<math>\partial f(x)(h)=xh+hx</math>
 
and the components are:
{| class="wikitable"
|-
| <math>\frac{{}_{(1)0}\partial x^2}{\partial x}=x\,\!</math>
| <math>\frac{{}_{(1)1}\partial x^2}{\partial x}=1\,\!</math>
|-
| <math>\frac{{}_{(2)0}\partial x^2}{\partial x}=1\,\!</math>
| <math>\frac{{}_{(2)1}\partial x^2}{\partial x}=x\,\!</math>
|}
 
Finally, for the function ''f''(''x'') = ''x''<sup>&minus;1</sup>, the derivative is
 
:<math>\partial f(x)(h)=-x^{-1}hx^{-1}</math>
 
and the components are:
{| class="wikitable"
|-
| <math>\frac{{}_{(1)0}\partial x^{-1}}{\partial x}=-x^{-1}\,\!</math>
| <math>\frac{{}_{(1)1}\partial x^{-1}}{\partial x}=x^{-1}\,\!</math>
|}
 
==References==
* [[Vladimir Arnold]] (1995) "The geometry of spherical curves and the algebra of quaternions", translated by [[Ian R. Porteous]], ''Russian Mathematical Surveys'' 50:1&ndash;68.
* C.A. Deavours (1973) "The Quaternion Calculus", [[American Mathematical Monthly]] 80:995&ndash;1008.
* [[Rudolf Fueter|R. Fueter]] (1936) "Über die analytische Darstellung der regulären Funktionen einer Quaternionenvariablen" (in German), [[Commentarii Mathematici Helvetici]] 8: 371&ndash;378.
* Graziano Gentili, Catarina Stoppato & D.C. Struppa (2013) ''Regular Functions of a Quaternionic Variable'', Birkhäuser, ISBN 978-3-642-33870-0.
* P.G. Gormley (1947) "Stereographic projection and the linear fractional group of transformations of quaternions", ''Proceedings of the [[Royal Irish Academy]]'', Section A 51: 67&ndash;85.
* K. Gürlebeck & W. Sprössig (1990) ''Quaternionic analysis and elliptic boundary value problems'', Birkhäuser ISBN 978-3-7643-2382-0 .
* W.R. Hamilton (1899) ''Elements of Quaternions'' v. I, edited by Charles Jasper Joly, "On differentials and developments of functions of quaternions", pages 430&ndash;64.
* R. Michael Porter (1998) [http://www.ams.org/journals/ecgd/1998-02-06/S1088-4173-98-00032-0/S1088-4173-98-00032-0.pdf Möbius invariant quaternion geometry], ''Conformal Geometry and Dynamics'' 2:89&ndash;196.  
* A. Sudbery (1979) "Quaternionic Analysis", ''Mathematical Proceedings of the Cambridge Philosophical Society'' 85:199&ndash;225.
 
[[Category:Quaternions]]
[[Category:Functions and mappings]]
[[Category:Articles containing proofs]]

Latest revision as of 21:20, 4 March 2014


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