Volume 2014, Issue 1 369430
Research Article
Open Access

The Regularity of Functions on Dual Split Quaternions in Clifford Analysis

Ji Eun Kim

Ji Eun Kim

Department of Mathematics, Pusan National University, Busan 609-735, Republic of Korea pusan.ac.kr

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Kwang Ho Shon

Corresponding Author

Kwang Ho Shon

Department of Mathematics, Pusan National University, Busan 609-735, Republic of Korea pusan.ac.kr

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First published: 17 April 2014
Citations: 1
Academic Editor: Zong-Xuan Chen

Abstract

This paper shows some properties of dual split quaternion numbers and expressions of power series in dual split quaternions and provides differential operators in dual split quaternions and a dual split regular function on Ω ⊂ 2 × 2 that has a dual split Cauchy-Riemann system in dual split quaternions.

1. Introduction

Hamilton introduced quaternions, extending complex numbers to higher spatial dimensions in differential geometry (see [1]). A set of quaternions can be represented as
(1)
where i2 = j2 = k2 = −1, ijk = −1, and denotes the set of real numbers. Cockle [2] introduced a set of split quaternions as
(2)
where , , and e1e2e3 = 1. A set of split quaternions is noncommutative and contains zero divisors, nilpotent elements, and nontrivial idempotents (see [3, 4]). Previous studies have examined the geometric and physical applications of split quaternions, which are required in solving split quaternionic equations (see [5, 6]). Inoguchi [7] reformulated the Gauss-Codazzi equations in forms consistent with the theory of integrable systems in the Minkowski 3-space for split quaternion numbers.

A dual quaternion can be represented in a form reflecting an ordinary quaternion and a dual symbol. Because dual-quaternion algebra is constructed from real eight-dimensional vector spaces and an ordered pair of quaternions, dual quaternions are used in computer vision applications. Kenwright [8] provided the characteristics of dual quaternions, and Pennestrì and Stefanelli [9] examined some properties by using dual quaternions. Son [10, 11] offered an extension problem for solutions of partial differential equations and generalized solutions for the Riesz system. By using properties of Hamilton operators, Kula and Yayli [4] defined dual split quaternions and gave some properties of the screw motion in the Minkowski 3-space, showing that has a rotation with unit split quaternions in and a scalar product that allows it to be identified with the semi-Euclidean space for split quaternion numbers.

It was shown (see [12, 13]) that any complex-valued harmonic function f1 in a pseudoconvex domain D of 2 × 2, being the set of complex numbers, has a conjugate function f2 in D such that the quaternion-valued function f1 + f2j is hyperholomorphic in D and gave a regeneration theorem in a quaternion analysis in view of complex and Clifford analysis. In addition, we [14, 15] provided a new expression of the quaternionic basis and a regular function on reduced quaternions by associating hypercomplex numbers e1 and e2. We [16] investigated the existence of hyperconjugate harmonic functions of an octonion number system, and we [17, 18] obtained some regular functions with values in dual quaternions and researched an extension problem for properties of regular functions with values in dual quaternions and some applications for such problems.

This paper provides a regular function and some properties of differential operators in dual split quaternions. In addition, we research some equivalent conditions for Cauchy-Riemann systems and expressions of power series in dual split quaternions from the definition of dual split regular on an open set Ω2 × 2.

2. Preliminaries

A dual number A has the form a + εb, where a and b are real numbers and ε is a dual symbol subject to the rules
(3)
and a split quaternion q𝒮 is an expression of the form
(4)
where xm  (m = 0,1, 2,3) and er  (r = 1,2, 3) are split quaternionic units satisfying noncommutative multiplication rules (for split quaternions, see [1]):
(5)
Similarly, a dual split quaternion z can be written as
(6)
which has elements of the following form:
(7)
where p0 = z0 + z1e2 and p1 = z2 + z3e2 are split quaternion components, z0 = x0 + x1e1, z1 = x2 + x3e1, z2 = y0 + y1e1, and z3 = y2 + y3e1 are usual complex numbers, and xm, ym  (m = 0,1, 2,3). The multiplication of split quaternionic units with a dual symbol is commutative εer = erε  (r = 1,2, 3). However, by properties of split quaternionic unit,
(8)
where
(9)
with , , , and . For instance,
(10)
Because of the properties of the eight-unit equality, the addition and subtraction of dual split quaternions are governed by the rules of ordinary algebra. Here the symbol p(kr) is used by just enumerating r and k, not r times k. For example, p(22)p4 and p22 = p4.
For any two elements z = p0 + εp1 and w = q0 + εq1 of 𝒟(𝒮), where and are split quaternion components and sr, tr  (r = 0,1, 2,3), their noncommutative product is given by
(11)
The conjugation z* of z and the corresponding modulus zz* in 𝒟(𝒮) are defined by
(12)
where and .

Lemma 1. For all z𝒟(𝒮) and n : = {1,2, 3, …}, we have

(13)

Proof. If n = 1, then (13) is trivial. Now suppose that this holds for some n. Then, as desired,

(14)

By the principle of mathematical induction, (13) holds for all n.

Let Ω be an open subset of 2 × 2. Then the function f : Ω𝒟(𝒮) can be expressed as
(15)
where the component functions fr : Ω𝒮  (r = 0,1) are split quaternionic-valued functions. The component functions fr  (r = 0,1) are
(16)
where gk = u2k + u2k+1e1  (k = 0,1) and gk = v2k−4 + v2k−3e1  (k = 2,3) are complex-valued functions, and ur and vr  (r = 0,1, 2,3) are real-valued functions.
Now, we let differential operators D1 and D2 be defined on 𝒟(𝒮) as
(17)
Then the conjugate operators and are
(18)
where
(19)
(20)
act on 𝒟(𝒮). These operators are called corresponding Cauchy-Riemann operators in 𝒟(𝒮), where /zr and are usual differential operators used in the complex analysis.

Remark 2. From the definition of differential operators on 𝒟(𝒮),

(21)
where r = 1,2.

Definition 3. Let Ω be an open set in 2 × 2. A function f = f0 + εf1 is called an Lr (resp., Rr)-regular function (r = 1,2) on Ω if the following two conditions are satisfied:

  • (i)

    fk  (k = 0,1) are continuously differential functions on Ω, and

  • (ii)

    (resp., ) on Ω  (r = 1,2).

In particular, the equation of Definition 3 is equivalent to
(22)
In addition,
(23)
Concretely, the following system is obtained:
(24)
The above systems (23) and (24) are corresponding Cauchy-Riemann systems in 𝒟(𝒮). Similarly, the equation of Definition 3 is equivalent to
(25)
Then,
(26)
Concretely, the following system is obtained:
(27)
The above systems (26) and (27) are corresponding Cauchy-Riemann systems in 𝒟(𝒮).
On the other hand, the equation of Definition 3 is equivalent to
(28)
Then,
(29)
where
(30)
Concretely, the following system is obtained:
(31)
Similarly, the equation of Definition 3 is equivalent to
(32)
Then,
(33)
where
(34)
Concretely, the system is obtained as follows:
(35)
From the systems (24), (27), (31), and (35), the equations and are different. Therefore, the equations and should be distinguished as Lr-regular functions (r = 1,2) and Rr-regular functions (r = 1,2) on Ω, respectively. Now the properties of the Lr-regular function (r = 1,2) with values in 𝒟(𝒮) are considered.

3. Properties of Lr-Regular Functions (r  =  1,2) with Values in 𝒟(𝒮)

We consider properties of a Lr-regular functions (r = 1,2) with values in 𝒟(𝒮).

Theorem 4. Let Ω be an open set in 2 ×  2 and let f = f0 +  εf1 = (g0 + g1e2) + ε(g2 + g3e2) be an L1-regular function defined on Ω. Then

(36)

Proof. By the system (23), we have

(37)
Therefore, we obtain
(38)

Theorem 5. Let Ω be an open set in 2 × 2 and f = f0 + εf1 = (g0 + g1e2) + ε(g2 + g3e2) be an L2-regular function defined on Ω. Then

(39)

Proof. By the system (26), we have

(40)
Therefore, we obtain the following equation:
(41)

Proposition 6. From properties of differential operators, the following equations are obtained:

(42)

Proof. By properties of the power of dual split quaternions and derivatives on 𝒟(𝒮), the following derivatives are obtained:

(43)
The other equations are calculated using a similar method, and the above equations are obtained.

Theorem 7. Let Ω be an open set in 2 × 2 and let f(z) be a function on Ω with values in 𝒟(𝒮). Then the power zn of z in 𝒟(𝒮) is not an L1-regular function but an L2-regular function on Ω, where n.

Proof. From the definition of the Lr-regular function (r = 1,2) on Ω and Proposition 6, we may consider whether the power zn of z in 𝒟(𝒮) satisfies the equation . Since ,

(44)
Hence, the power zn of z is not L1-regular on Ω. On the other hand, from the equations in Proposition 6, we have , , and . Then,
(45)
Therefore, by the definition of the Lr-regular function (r = 1,2) on Ω, a power zn of z is L2-regular on Ω.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

The second author was supported by the Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Science, ICT, and Future Planning (2013R1A1A2008978).

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