Research Article | Open Access

Volume 2009 |Article ID 923809 | https://doi.org/10.1155/2009/923809

Xiaoqin P. Wu, "Simple-Zero and Double-Zero Singularities of a Kaldor-Kalecki Model of Business Cycles with Delay", Discrete Dynamics in Nature and Society, vol. 2009, Article ID 923809, 29 pages, 2009. https://doi.org/10.1155/2009/923809

# Simple-Zero and Double-Zero Singularities of a Kaldor-Kalecki Model of Business Cycles with Delay

Academic Editor: Xue-Zhong He
Received12 Aug 2009
Accepted02 Nov 2009
Published03 Feb 2010

#### Abstract

We study the Kaldor-Kalecki model of business cycles with delay in both the gross product and the capital stock. Simple-zero and double-zero singularities are investigated when bifurcation parameters change near certain critical values. By performing center manifold reduction, the normal forms on the center manifold are derived to obtain the bifurcation diagrams of the model such as Hopf, homoclinic and double limit cycle bifurcations. Some examples are given to confirm the theoretical results.

#### 1. Introduction

In the last decade, the study of delayed differential equations that arose in business cycles has received much attention. The first model of business cycles can be traced back to Kaldor  who used a system of ordinary differential equations to study business cycles in 1940 by proposing nonlinear investment and saving functions so that the system may have cyclic behaviors or limit cycles, which are important from the point of view of economics. Kalecki  introduced the idea that there is a time delay for investment before a business decision. Krawiec and Szydłowski  incorporated the idea of Kalecki into the model of Kaldor by proposing the following Kaldor-Kalecki model of business cycles:

where is the gross product, is the capital stock, is the adjustment coefficient in the goods market, is the depreciation rate of capital stock, and are investment and saving functions, and is a time lag representing delay for the investment due to the past investment decision. This model has been studied extensively by many authors; see . Several authors also discussed similar models  and established the existence of limit cycles.

Considering that past investment decisions  also influence the change in the capital stock, Kaddar and Talibi Alaoui  extended the model (1.1) by imposing delays in both the gross product and capital stock. Thus adding the same delay to the capital stock in the investment function of the second equation of Sys. (1.1) leads to the following Kaldor-Kalecki model of business cycles:

As in ; also see [10, 16, 17], using the following saving and investment functions and , respectively, where and are constants, we obtain the following system:

Kaddar and Talibi Alaoui  studied the characteristic equation of the linear part of Sys. (1.4) at an equilibrium point and used the delay as a bifurcation parameter to show that the Hopf bifurcation may occur under some conditions as passes some critical values. However, they did not obtain the stability of the bifurcating limit cycles and the direction of the Hopf bifurcation. Wang and Wu  further studied Sys. (1.4) and gave a more detailed discussion of the distribution of the eigenvalues of the characteristic equation which has a pair of purely imaginary roots. They derived the normal forms on the center manifold for sys. (1.4) to give the direction of the Hopf bifurcation and the stability of the bifurcating limit cycles for some critical values of .

However, under certain conditions, the characteristic equation of the linear part of Sys. (1.4) may have a simple-zero root, a double-zero root, or a simple zero root and a pair of purely imaginary roots. In this paper, simple-zero (fold) and double-zero (Bogdanov-Takens) singularities for Sys. (1.4) and their corresponding dynamical behaviors are investigated by using and as bifurcation parameters (where is defined in Section 2). The discussion of zero-Hopf singularity will be addressed in a coming paper.

The rest of this manuscript is organized as follows. In Section 2, a detailed presentation is given for the distribution of eigenvalues of the linear part of Sys. (1.4) at an equilibrium point in the -parameter space. In Section 3, the theory of center manifold reduction for general delayed differential equations (DDEs) is briefly introduced. In Sections 4 and 5, center manifold reduction is performed for Sys. (1.4); and hence, the normal forms for simple-zero and double-zero singularities are obtained on the center manifold, respectively. In Section 6, the normal forms for the double-zero singularity are used to predict the bifurcation diagrams such as Hopf, homoclinic, and double limit cycle bifurcations for the original Sys. of (1.4). Finally in Section 7, some numerical simulations are presented to confirm the theoretical results.

#### 2. Distribution of Eigenvalues

Throughout the rest of this paper, we assume that

and that is an equilibrium point of Sys. (1.4). Let , , , and . Then Sys. (1.4) can be transformed as

Let the Taylor expansion of at 0 be

where

The linear part of Sys. (2.2) at is

and the corresponding characteristic equation is

where

For , (2.6) becomes

Define

Theorem 2.1. Let . If , then all roots of (2.8) have negative real parts, and hence is asymptotically stable. If , then (2.8) has a positive root and a negative root, and hence, is unstable.

Now assume . Clearly if and only if . Next we always assume that . It is easy to attain

Define . Then we have that,

Define

Hence if , , and hence , and if , , and hence if and only if . Also if and only if . Thus we obtain the following result.

Lemma 2.2. Suppose that . Then the following are considered. (i)If , then (2.6) has a simple root 0 for all . (ii)Let . Then the following are given. (a)Equation (2.6) has a simple root 0 if and only if , (b)Equation (2.6) has a double root 0 if and only if and .

Let () be a purely imaginary root of (2.6). After plugging it into (2.6) and separating the real and imaginary parts, we have that

Adding squares of two equations yields Then (2.14) has a nonzero solution if and only if and does not have a nonzero solution if and only if . If , from (2.14), we solve as follows:

and from (2.13), we solve , as:

Define

From (2.16), we obtain

Clearly if , then has two positive roots, and if , then . Now, under , we impose the following conditions:

(H1), , (H2), , , (H3), , , (H4), , ,(H5), , ,(H6), , ,(H7), , .

Based on Lemma 2.2, we have the following result.

Lemma 2.3. Suppose that and . Then the following are obtained.(i)Under one of the conditions (H1), (H2), and (H4), (2.6) has a simple zero root and does not have other roots in the imaginary axis.(ii)Under the condition (H5), (2.6) has a simple zero root and a pair of purely imaginary roots in the imaginary axis if , (iii)Under one of the conditions (H3) and (H6), then (2.6) has a double root 0 and does not have other roots in the imaginary axis. (iv)Under the condition (H7), (2.6) has a double zero root and a pair of purely imaginary roots in the imaginary axis if for some .

Now we use the roots of , to give a more detailed discussion for the roots of (2.6). Define

Clearly is the positive root of and , are two positive roots of if . Note that if if , if , or then if . Also note that as well as if , . In fact it is based on the following calculation:

Thus for , we always have . Noting that , we have the following result.

Lemma 2.4. Let . Then the following are given.(i)Suppose that . Then for , then (2.6) has a simple zero root and does not have roots in the imaginary axis. (ii)Suppose that . If , then (2.6) has a simple zero root and does not have roots in the imaginary axis. And if , (2.6) has a double zero root and does not have roots in the imaginary axis. (iii)Suppose that . If , then (2.6) has a simple zero root and does not have roots in the imaginary axis. If , then (2.6) has a double zero root and does not have roots in the imaginary axis. And if , then (2.6) has a double zero root and has a pair of purely imaginary roots. (iv)Suppose that . Then if , then (2.6) has a simple zero root and does not have roots in the imaginary axis. If , then (2.6) has a double zero root and does not have roots in the imaginary axis. If , then (2.6) has a double zero root and has a pair of purely imaginary roots when for some . And if , (2.6) has a double zero root and does not have a pair of purely imaginary roots.

Define to be the root of (2.6) such that and . Then we have the following result.

Lemma 2.5. Suppose that and . Then .

Proof. Differentiating (2.6) with respect to yields and a simple calculation gives which gives thus completing the proof.

Next we discuss the distribution of other roots of (2.6). We need the following lemma due to Ruan and Wei .

Lemma 2.6. Consider the exponential polynomial where , are real polynomials such that and . As varies, the sum of the order of zeros of on the open right half-plane can change only if a zero appears on or crosses the imaginary axis.

Lemma 2.7. Let and . Then, the following are obtained.(i)If , then all roots of (2.6) except 0 and purely imaginary roots have negative real parts,(ii)If , then (2.6) has at least one positive root.

Proof. Note that, for , if or , has a zero root and a negative root. Using Lemmas 2.2 and 2.6, we obtain claim (i). For , has a zero root and a positive root if or . For , let Also noting that when , we have that and . This proves the second part of the lemma and completes the proof of the lemma.

#### 3. Center Manifold Reduction

In this section, we briefly summarize the theory of center manifold reduction for general DDEs. The material is mainly taken from [20, 21]. Consider the following DDE:

where , . This equation is equivalent to

which can be written as

where , , and . Define with supreme norm and is defined by , ; is a bounded linear operator; and is a function with , . Consider the following linear system:

Since is a bounded linear operator, then can be represented by a Riemann-Stieltjes integral

by the Riesz representation theorem, where () is an matrix function of bounded variation. Let be the infinitesimal generator for the solution semigroup defined by Sys. (3.4) such that

Define the bilinear form between and (where is the space of all row -vectors) by

The adjoint of is defined by as

In our setting, (3.3) has trivial components. Assume that the characteristic equation of (3.3) has eigenvalue zero with multiplicity and all other eigenvalues have negative real parts. Then has a generalized eigenspace which is invariant under the flow (3.4). Let be the space adjoint with in . Then can be decomposed as where , . Choose the bases and for and , respectively, such that

where is Jordan matrix associated with the eigenvalue 0.

To consider Sys. (3.3), we need to enlarge the space to the following :

The elements of can be expressed as with and

where is the identity matrix. Define the projection by

Then the enlarged phase space can be decomposed as Let with and . Then (3.3) can be decomposed as

where is an extension of the infinitesimal generator from to , defined by

for and its adjoint by is defined by

for . Let . Then Sys. (3.13) becomes

where

On the center manifold, (3.16) can be approximated as

#### 4. Simple-Zero Singularity

In this section, we assume that the condition (H2) holds. From the definition of , we know that if and only if . Therefore (H2) is equivalent to

From (ii) of Lemma 2.4 and (ii) of Lemma 2.7, we know that, at , the characteristic equation of the linear part of Sys. (2.5) has a simple zero root and the rest of roots have negative parts. We treat as a bifurcation parameter near .

Set , . Let . Then Sys. (2.5) can be rewritten as

The linearization of Sys. (4.2) at is

Let where

Let and

Define

Then Sys. (4.2) becomes

From (3.7), the bilinear form can be expressed as

It is not hard to see that the infinitesimal generator is given by

for and its adjoint by

for .

Next we obtain the bases for the center space and its adjoint space , respectively. Let for , that is,

then we know that is a constant vector such that

Then we have two linearly independent solutions , which are bases for the center space . Let .

Similarly, let for , that is,

then we know that is a constant vector such that From this we have two linearly independent solutions and which are bases for the center space . Let with being determined such that . In fact

Clearly is well defined since . It is not hard to check that , and , where .

Let . Then Sys. (4.2) can be decomposed as

Write . Note that

Here represents higher-order terms. Thus, for sufficiently small , on the center manifold, if , then Sys. (4.2) becomes

If and , then Sys. (4.2) can be transformed into the following form:

Thus we have the following results.

Theorem 4.1. Let be small. Then consider what follows.(i)Suppose that . Then if , the equilibrium is unstable, and if and , then the equilibrium is asymptotically stable for and unstable if .(ii)The equilibrium is asymptotically stable if and unstable if .(iii)At , Sys. (1.4) undergoes a transcritical bifurcation if and a pitchfork bifurcation if and .

#### 5. Double-Zero Singularity

In this section, we assume that one of the conditions (H3) and (H6) holds and , or equivalently, as

From Section 2, we can see that, at , the characteristic equation of Sys. (2.5) has a double root 0 and all other roots have negative real parts if and . We treat as a bifurcation parameter near .

By scaling , Sys. (2.2) can be written as

Let . Let , . Then on we have

The linearization of Sys. (5.3) at is

Let

where

Define

Let . Let and where

Then Sys. (5.3) can be transformed into

Let . From (3.7), the bilinear inner product between and can be expressed by

for and . As in Section 4, the infinitesimal generator associated with is given by

for and its adjoint by

for . From Section 2, we know that is an eigenvalue of and with multiplicity 4. Now we compute eigenvectors of and associated with , respectively.

Next we obtain the bases for the center space and its adjoint space , respectively. Let for . This means that

From this we obtain that is a constant vector in satisfying

This equation has three linearly independent solutions: , , . Let be one of those. Suppose that for , namely,

This implies that there is a constant vector in such that and

Since

we have that

It is easy to see that (5.18) has no solution if is either or . For , setting in (5.18), we obtain and hence . Thus we obtain bases , , , for the center space . Let . Then we have that where .

Similarly, let for , that is,

which means that is a constant vector satisfying

This equation has three linearly independent solutions: , , . Asserting that gives

Let be one of , , . Suppose , that is,

which implies that there is such that satisfying

Since

we have

It is not hard to check that (5.26) has no solution if or . Letting , setting in (5.26) and using , we can get and :

Hence

Then , , , are bases of the center space . Let . Then , and .

Let , namely,

Then Sys. (5.9) can be decomposed as

Write . Then, on the center manifold, Sys. (5.30) becomes

where

Next we use techniques of nonlinear transformations in  to transform Sys. (5.31) into normal forms. If , then up to the second order, Sys. (5.31) can be written as