In this paper, we propose complex uncertain differential equations (CUDEs) based on uncertainty theory. In order to describe the evolution of complex uncertain phenomenon related to belief degrees, we apply the complex Liu process to CUDEs. Firstly, we pose a concept of a linear CUDE and prove that homogeneous linear CUDE and general linear CUDE have solutions. Then, we prove existence and uniqueness theorem of a special CUDE. Further, we design a numerical algorithm to obtain inverse uncertainty distribution of the solution. Finally, as an application, we analyse the inverse uncertainty distributions of time integral of CUDEs and design numerical algorithms to obtain inverse uncertainty distributions of time integral.
Differential equation [1, 2] is a classic mathematical branch and plays a very important role in formulation and analysis in modern nature and social sciences. The existence of randomness and fuzziness in dynamic systems brought stochastic differential equations and fuzzy differential equations which have been widely applied in various sciences, such as physical [3], mathematics [4, 5], control model [6], epidemic model [7], economics [8] and finance [9] and other fields. However, the complexity of the world makes the events we face uncertain in various forms. In the real life, some information and knowledge, which usually are represented by human language like about 100km, approximately 39°C, roughly 80kg, low speed, middle age, and big size, behave neither like randomness nor like fuzziness. In order to deal with this type of uncertainty, we need a new theory called uncertainty theory to replace randomness and fuzziness.
Uncertainty theory goes back to a series of papers [10, 11] by the mathematician B. Liu in the past decade. Uncertainty theory as a perfect axiomatic system provides us an alternative for modeling human uncertainty without the scope of probability theory. Probability is interpreted as a frequency that requires enough historical data for probabilistic reasoning, while uncertainty is interpreted as personal belief degree that is from domain experts for lack of samples. Until now, a number of authors have considered the effects of uncertainty theory in various fields (for example, Liu [12]; Gao et al. [13]; Wang et al. [14]; Li et al. [15]).
In 2008, in order to describe the evolution of uncertain phenomenon related to belief degrees, Liu [16] first proposed uncertain differential equation for describing dynamic uncertain systems. Later, in 2009, Liu [17] claimed Liu process is an uncertain process with stationary and independent normal uncertain increments. Chen and Liu [18] considered the analytic solution of a linear uncertain differential equation in 2010. After that, Gao [19] proved the existence and uniqueness theorem of uncertain differential equation. Furthermore, the special nonlinear uncertain differential equations were solved in 2013(for example, Liu et al. [20]; Yao et al. [21]; Liu et al. [22]; Wang et al. [23]). More importantly, Yao and Chen [24, 25] developed a numerical method to obtain the inverse uncertainty distributions of solution of an uncertain differential equation. Based on above theoretical development, uncertain differential equation has been successfully applied in many fields (for example, Yang et al. [26, 27]; Gao et al. [28–30]; Jia et al. [31–33]). Of course, there are still many literatures about the fields of uncertain differential equations, which will not be listed here.
In the field of systems analysis, signal analysis, anomalous integral, finance analysis, quantum mechanics, relativity, fluid mechanics and so on, some quantities needed to be characterized by complex numbers, such as root locus method of systems analysis, periodic signals of signal analysis, metric equation of relativity, and two-dimensional potential flow of fluid mechanics. When we face with the lack of measuring methods, experimental conditions etc., we tend to determine the quantities by subjective methods. Complex random variable and fuzzy complex number have been employed to model these quantities. However, a lot of literatures (such as Liu [10, 11]) show that probability theory and fuzzy theory are not enough for all the problems. Under the framework of uncertainty theory, Peng [34] proposed the concept of complex uncertain variable and studied some properties including independence, distribution, expected value and variance. In order to describe complex uncertain process, the concept of complex uncertain distribution and some properties of complex uncertain integral were presented by You et al. [35]. After that, Chen et al. [36] investigated the convergence of complex uncertain sequences including convergence almost surely, in measure,in mean, convergence in distribution and uniformly almost surely and relationships among them. Chen et al. [37] further proposed the concepts of pseudo-variance of a complex uncertain variable and calculated the variance and the pseudo-variance by inverse uncertainty distributions of the real and imaginary parts of complex uncertain variable. In the same year, Gao et al. [38] extended complex uncertain variable to complex uncertain random variables. However, to our best knowledge, the research on complex uncertain differential equation has not been carried out so far.
The paper is organized as follows: In Section 2, we recall some basic definitions and theorems of uncertainty theory, the definitions of complex uncertain process, the expected value and so on. Section 3 demonstrates the existence and uniqueness theorem of complex uncertain differential equation. Section 4 give inverse uncertainty distribution of time integral of complex uncertain differential equation and two numerical examples. Finally a brief conclusion is given in Section 5.
Preliminaries
In this section, we will recall some fundamental concepts and properties concerning uncertain variables, uncertain expected value, uncertain processes, complex uncertain expected value, complex uncertain processes and so on.
Definition 2.1. [11] An uncertain variable is a measurable function ξ from an uncertainty space to the set of real numbers, i.e., for any Borel set B of real numbers, the set
is an event.
Definition 2.2. [11] Let ξ be an uncertain variable. Then the expected value of ξ is defined by
provided that at least one of the two integrals is finite.
An uncertain process is essentially a sequence of uncertain variables indexed by time.
Definition 2.3. [11] Let T be an index set and let be an uncertainty space. An uncertain process is a measurable function from to the set of real numbers such that {Zt ∈ B} is an event for any Borel set B for each time t.
Definition 2.4. [11] An uncertain process Ct with respect to time t is said to be a Liu process if
(i) C0 = 0 and almost all sample paths are Lipschitz continuous,
(ii) Ct has stationary and independent increments,
(iii) every increment Cr+t - Cr is a normal uncertain variable with expected value 0 and variance t2, whose uncertainty distribution is
Definition 2.5. [11] Let Zt be an uncertain process and Ct be a Liu process. For any partition of closed interval [a, b] with a = t1 < t2 < ⋯ < tn+1 = b, the mesh is written as
Then uncertain integral of Zt with respect to Ck is
provided that the limit exists almost surely and is finite. In this case, the uncertain process Zt is said to be integrable.
Definition 2.6. [11] Let Zt be an uncertain process and Ct be a Liu process. If there exist two processes μt and σt such that
Then Zt is called a uncertain process with drift μt and diffusion σt. Furthermore, Zt has an uncertain differential
Definition 2.7. [11] Suppose that Ct is a Liu process, f and g are continuous functions. Given an initial value Z0, the uncertain differential equation
is called an uncertain differential equation with an initial value Z0.
Theorem 2.1.[16] Let Zt and be the solution and α-path of the uncertain differential equationThen
Lemma 2.1.[18] Suppose that Ct is a Liu process, and Zt is an integrable uncertain process on [a, b] with respect to t. Then the inequalityholds, where K (γ) is the Lipschitz constant of the sample path Zt (γ).
Definition 2.8. [34] An complex uncertain variable is a function from an uncertainty space to the set of complex numbers.
Definition 2.9. [35] Let T be an index set and let be an uncertainty space. A complex uncertain process is a function from to the set of complex numbers for each time t.
Theorem 2.2.[35] A uncertain process Zt is complex if and only if there exist two uncertain processes Z1k and Z2k such that
Definition 2.10. [35] Let C1k and C2t be two independent Liu processes. Then the complex uncertain process Ct = C1t + iC2t is called a complex Liu process. In particular, a complex Liu process Ct = C1t + iC2t is said to be standard if C1t and C2t are both standard Liu processes.
Definition 2.11. [35] Let Zt = Z1t + iZ2t be a complex uncertain process and let
be a standard complex Liu process. Then the complex uncertain integral of Zt with respect to Ct is defined by
Theorem 2.3.[35] If Zt = Z1t + iZ2t is a complex uncertain process, Z1t and Z2t are two continuous uncertain processes, and Ct = C1t + iC2t is a complex Liu process, then exists and
Definition 2.12. [35] The complex uncertain distribution ϒ of a complex uncertain variable ξ is defined by
for any complex number z = z1 + iz2, Definition 2.13. [35] Complex uncertain process Zt is said to have a complex uncertainty distribution ϒt (z) if at each fixed time , complex uncertain variable has complex uncertainty distribution , the inverse function is called the inverse uncertainty distribution of Zt.
Theorem 2.4.[35] A function ϒt (z) : T × C ↦ [0, 1] is a complex uncertainty distribution of complex uncertain process if and only if at each time t, it is monotone increasing with respect to the real part Re (z) and imaginary part Im (z), respectively, and
and
Definition 2.14. [37] If the real and imaginary parts of complex uncertain process Zt exist, then the expected value of Zt is defined by
Theorem 2.5.[37] Let Zt be a complex uncertain process. Assume Re [Zt] and Im [Zt] are independent uncertain variables with regular uncertainty distributions Φ and Ψ, respectively. Then
Some classes of CUDEs
Linear CUDEs
Definition 3.1. Let Zt = Z1t + iZ2t be a complex uncertain process, let Ct = C1t + iC2t be a complex Liu process. Then
is called a linear CUDE, where δt, ζt, σt, ηt are given complex uncertain processes. If δt = 0, σt = 0, we call it homogeneous.
Theorem 3.1.Suppose Ct = C1t + iC2t is a complex Liu process. If ζt, ηt are complex uncertain processes, then homogeneous linear CUDE
has a solution
Proof. By Theorem 4 of [17], it holds that
Taking integration on both sides of the above equation, we can get
So, the solution of (1) is
□
Corollary 3.1.Linear CUDE
has a solution
Proof. Let
where
Set X0 = 1 and Y0 = Z0 . According to Theorem 4 of [17], taking the differentials on both sides of Zt = XtYt, it holds that
It follows from the solution of (1) in Theorem 3.1 that
which means
□
Example 3.1. Let Ct be a standard complex Liu process. And complex uncertain process Zt is given as follows
By Theorem 3.1, we get
that is
Example 3.2. Let η, a, b be real number. For the following nonlinear CUDE,
At first,we have
It follows from Corollary 3.1 that the solution is
That is,
provided that a ≠ 0. Note that Zt is a normal complex uncertain variable,i.e.,
and
Existence and uniqueness theorem of CUDEs
Lemma 3.1.Suppose that Ct = C1t + iC2t is a complex Liu process, and Zt is an integrable uncertain process on [a, b] with respect to t. Then the inequalityholds, where K (γ) is the larger Lipschitz constant of C1t and C2t.
Proof. Let a = t1 < t2 < ⋯ < tn+1 = b, Then uncertain integral of Zt with respect to Ct is . By the definition of uncertain integral and complex uncertain integral, we get
For each sample γ, it follows from the definition of Liu process that Ct (γ) is Lipschitz continuous with respect to time t . Then there exists a larger Lipschitz constant K (γ) of C1t and C2t such that
Thus
□
Theorem 3.2.The following CUDE
has a unique solution and the solution is sample-continuous, where Ct = C1t + iC2t and the coefficients f (z, t) and g (z, t) satisfy the following Lipschitz condition and linear growth condition for some constants L, T, and
Proof.Step 1. (existence), we consider approximation method to construct a solution of the CUDE (7). Define and
For any sample γ, we define
We claim that
where T is a constant. Indeed for n = 0, it follows from Lemma 3.1 that
This confirms the claim for n = 0 . Next we assume the claim is true for some n - 1 . Then
Since
we have is convergent uniformly in t ∈ [0, T] . Denote the limit by Zt (γ) , we have
By the proof above, for each γ with Ct (γ) >0, we get
Step 2. (sample continuity), for ɛ > 0, there exists
when t > r and |t - r| < δ, we have
Thus the solution of (7) is sample-continuous.
Step 3. (uniqueness), we assume that both of Zt and are solutions of (7). Then for any γ ∈ Γ with Ct (γ) >0, we have
Gronwall inequality implies the uniqueness. The proof is completed.□
Example 3.3. Considering the following CUDE
where C1t, C2t are standard Liu processes,
In this example, f = a . It is obvious that f = a is Lipschitz continuous function. According to Theorem 3.2, the solution of (8) exists and is unique. In fact, we have
Example 3.4. Considering the following CUDE
where C1t, C2t are standard Liu processes,
In this example, f = az . Since we know f = az is Lipschitz continuous function. According to Theorem 3.2, the solution of (9) exists and is unique. In fact, we have
Example 3.5. Considering the following linear CUDE
According to Theorem 3.2, in this example,
Thus
and
Taking
and
So, the solution of linear CUDE of this example exists and is unique. It follows from Corollary 3.1 that the unique solution is
Numerical method
In this subsection, we generalize the Yao-Chen formula [24] to the CUDE. Let α be a number with 0 < α < 1, and let Ct = C1t + iC2t be complex Liu process. An CUDE
is said to have an α-path if it solves the corresponding complex ordinary differential equation:
where Φ-1 (α) is the inverse uncertainty distribution of standard normal uncertain variable i.e.,
Example 3.6. Let a, b be real numbers. The CUDE:
has an α-path:
Lemma 3.2.Assume that f, g are continuous functions of two variables and Ct = C1t + iC2t is complex Liu process. Let Zt and be the solution and α-path of the CUDE:respectively. Then we get
Proof. For each α-path we construct sets as follows,
It is obvious that T+∩ T- = ∅ and T+ ∪ T- = [0, + ∞).
Write
where Φ-1 (α) is the inverse uncertainty distribution of Since T+ and T- are disjoint sets and Cjt have independent increments, we get
we always have
Let . Because Ct = C1t + iC2t, then, we have
That is,
So, it holds that
Hence, we have
On the other hand, write
Since T+ and T- are disjoint sets and Cjt have independent increments, we get
we always have
Let Because Ct = C1t + iC2t, then, we have
That is
So, it holds that
Hence, we have
Since and are opposite events with each other. It follows from the duality axiom that
It follows from
and monotonicity theorem that
Thus, the results follow from (1)0, (1)1, and (1)21. □
Theorem 3.3.Assume that f, g are continuous functions of two variables and Ct = C1t + iC2t. Let Zt and be the solution and α-path of the CUDE:
respectively. Then, the solution Zt has an inverse uncertainty distribution:
Proof. Obviously,
It follows from the monotonicity theorem and Lemma 3.2 that:
Similarly, we also obtain
Since and are opposite events with each other. Besides, by using the duality axiom, we have:
It follows from (1)2, (1)3, and (1)4 that:
that is, The proof is completed. □
To calculate the inverse uncertainty distribution of the solution, we design a numerical algorithm as follow.
Inverse uncertainty distribution (IUD) of the solution
Algorithm 3.1
Let be an initial guess.
Step 1
Set α = 0, step length Δα.
Step 2
α = α + Δα
Step 3
Fix l as the step length. Set j = 0,and
for a fixed α in (0,1)
Step 4
Use the recursion formula
and calculate
Step 5
Set j ← j + 1 .
Step 6
Repeat Step 4 and Step 5 for N times.
Step 7
Obtain the IUD Zt for α.
Step 8
Return to step 2, while α + Δα < 1 .
Step 9
Output the iterative results. Then obtain
the IUD at each α in (0,1).
Step 10
The expected value at time T is
Remark 3.1. For the outer loop, for each α in (0,1), break up α in (0,1), if we suppose the number of shares is M. While the internal time complexity is O (N). So the time complexity of this algorithm becomes .
Example 3.7. Let a, b be real numbers and let Ct = C1t + iC2t be complex Liu process. The uncertain differential equation:
has a solution:
with an inverse uncertainty distribution:
In order to illustrate the numerical method, let a = 1, b = 1,then
whose solution is Zt = exp(t + C1t + iC2t) .
The α-path of Equation (1)5 is
Based on the Algorithm 3.1 we design (see Table 1), we obtain the running time of this example is 8.23088806s. The inverse uncertainty distribution of Zt is shown in Fig. 1. At the same time, we give the analytic solution as a comparison in Fig. 1. The error of the real part is 2.8802, the error of the imaginary part is 3.5553. And we can get
The IUD simulatin of Zt about CUDE.
Applications
In this section, we will give CUDEs applied in time integral, that is the inverse uncertainty distribution of time integral.
Inverse uncertainty distribution of time integral
Theorem 4.1.Let Zt and be the solution and α-path of the CUDE,respectively. For C (z) is a strictly increasing function. Then the integralhave the IUDfor C (z) is a strictly decreasing function. Then the integralhave the IUD
Proof. When C (z) is a strictly increasing function with respect to z, it is always true that
and
By Lemma 3.2, we obtain
Similarly, we have
It follows that
In other words, has an inverse uncertainty distribution
Similarly, for a strictly decreasing function C (z), it is always true that
and
By Lemma 3.2, we obtain
Similarly, we have
It follows that
In other words, has an inverse uncertainty distribution we can get the conclusion. □
To calculate the inverse uncertainty distribution of the integral of C (Zt), we design a numerical algorithm for two situations as follow.
The situation about a strictly increasing function C (z)
Algorithm 4.1
Let be an initial guess.
Step 1
Set α = 0, step length Δα.
Step 2
α = α + Δα
Step 3
Fix l as the step length. Set j = 0,
for a fixed α in (0,1)
Step 4
Use the recursion formula
and calculate and
Step 5
Set j ← j + 1 .
Step 6
Repeat Step 4 and Step 5 for N times.
Step 7
Obtain the IUD
for α.
Step 8
Return to step 2, while α + Δα < 1 .
Step 9
Output the iterative results.
Then the IUD
at each α in (0,1).
The situation about a strictly decreasing function C (z)
Algorithm 4.2
Let be an initial guess.
Step 1
Set α = 0, step length Δα.
Step 2
α = α + Δα
Step 3
Fix l as the step length. Set j = 0,
for a fixed α in (0,1)
Step 4
Use the recursion formula
and calculate and
Step 5
Set j ← j + 1 .
Step 6
Repeat Step 4 and Step 5 for N times.
Step 7
Obtain the IUD
for α.
Step 8
Return to step 2, while α + Δα < 1 .
Step 9
Output the iterative results.
Then the IUD
at each α in (0,1).
Remark 4.1. Similar to algorithm 1, algorithm 2 and 3 have similar time complexity. For the outer loop, for each α in (0,1), break up α in (0,1), if we suppose the number of shares is M. While the internal time complexity is O (N). So the time complexity of this algorithm becomes .
Numerical examples
Example 4.1. Let η, a, b be real number. For the following nonlinear CUDE,
with given initial value Z0 = 1 . The α-path equivalent equation of Equation (1)6 is
(i) Consider the time integral
where δ and H are real numbers. The α-path of Equation (1)7 is
for given times T > 0 . We set η = 5, a = 1, b = 2, t = 0.9 and N = 1, 000 . in Equation (1)6 and choose the parameters δ = 0.02 and H = 1 in Equation (1)8. Based on the Algorithm 4.1 we design (see Table 2), the IUD of time integral at T = 0.9 is shown in Fig. 2. The running time of this example is 8.68379906s.
The time integral simulatin of CUDE when C (z) is a strictly increasing function.
(ii) Consider the time integral
where δ and H are real numbers. The α-path of Equation (1)9 is
for given times T > 0 . We set η = 5, a = 1, b = 2, t = 0.9 and N = 1, 000 . in Equation (1)6 and choose the parameters δ = 0.02 and H = 1 in Equation (19). Based on the Algorithm 4.2 we design (see Table 3), the inverse uncertainty distribution of time integral at T = 0.9 is shown in Fig. 3. The running time of this example is 8.72653301s.
The time integral simulatin of CUDE when C (z) is a strictly decreasing function.
Conclusions
This paper mainly discussed existence and uniqueness theorem, numerical algorithm and time integral of CUDEs. First of all, we proposed the concepts of some classes of CUDEs. Furthermore, from the definition of CUDE, deduced existence, uniqueness, α-path, inverse uncertainty distributions successively, thus designing the numerical algorithm. Some analytic examples and numerical examples were provided to illustrate existence, uniqueness, inverse uncertainty distributions. Future researches may consider stability analysis and some applications in control fields.
Footnotes
Acknowledgments
The research was supported by Postgraduate Research & Practice Innovation Program of Jiangsu Province (KYCX20-0170).
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