• No results found

Corollary 3: Besides stability (stable node or stable focus), as identified through

5. Final remarks

t

k and ~ 0.2

t

k ,

respectively.

In both cases, the average of the time series is below zero, which is the steady state result in the absence of fluctuations. Thus, one may infer that the cycles are the result of an inefficient response of individuals to the economic conditions they perceive in each moment. The proposed model generates inefficient endogenous business cycles over the benchmark growth models, which do not take in consideration any ability of consumers to respond to the economic behaviour they witness.

5. Final remarks

In this paper, we have asked a simple question: what if agents react to last periods’

economic performance when making consumption decisions today? After all, economists unanimously consider that economic performance is directly attached to consumer confidence. If households are optimistic about the ability of the economy to grow above normal standards, they will be more willing to consume, and therefore the marginal propensity to consume out of income rises. If consumers are pessimistic, the opposite effect should be observed. Thus, we contrast the standard growth model under which agents believe that output converges in the long term to its potential level and act according to such belief, with a framework where agents are essentially myopic in the

sense they react to observable economic results rather than to a far in time benchmark that they do not have any guarantee to hold.

The proposed setup leads to endogenous business cycles that are triggered by households’ behaviour; if agents did not respond to cycles, these would just fade out.

Taking this argument seriously means that countercyclical economic policy may be adequate to attenuate the persistence of economic fluctuations; if agents do not perceive that the economy departs from the potential output level, then they will adjust savings rates obeying only to requisites of optimality under a frictionless scenario. Another major conclusion is that cycles are inefficient, in the sense that the economy will, on average, be worse off with than without them (our numerical examples point in this direction). Cycles penalize long term welfare, and therefore private agents should be educated not to give a strong response to short run fluctuations with regard to their decisions on the allocation of income between consumption and savings.

Appendix

Proof of proposition 1: Section 2 has defined the steady state as the long run locus that satisfies condition kkˆt+ =kˆt =kˆt =...=kˆtn

1

1 . Applying this condition to equation (2), one gets

[ ] functional form of the production function

Proof of proposition 2: The proposition states a trivial definition of stability;

thus, this prove only involves clarifying that the presented characteristic polynomial )

PJ is in fact the polynomial under which condition PJ(λ)=0 allows for the determination of the n+1 eigenvalues of matrix J (λj, j=1,…,n+1).

A characteristic polynomial is generically defined as ) Dividing all terms by the determinant, we continue to have a polynomial that allows for finding exactly the same n+1 solutions; thus, we define

) 1

Replacing the trace, the sums of the principal minors and the determinant that we have computed for our linearized system in the above polynomial, we find the expression in the proposition

Proof of proposition 3: Given the values of the trace and determinant of J, one verifies that 1+Tr(J)+Det(J)>0 and 1-Tr(J)+Det(J)<0, independently of parameter values. Relatively to the condition 1-Det(J)=0, that defines a Neimark-Sacker bifurcation, this is equivalent to the expression in item a) of the proposition. Local stability and local instability conditions are obtained by solving, respectively, Det(J)<1 and Det(J)>1

Proof of proposition 4: For n=2, the trace of the Jacobian matrix is equal to 1 (and, thus, the three eigenvalues associated with the Jacobian matrix cannot be all negative values); the determinant is negative (what implies that an odd number of negative eigenvalues exists). The two previous conditions imply with certainty that

0

Considering simultaneously the three above conditions implies that all the eigenvalues will lie inside the unit circle, that is, we guarantee stability. The three conditions may be rewritten as

(a) 1+Tr(J)+∑M×2(J)+Det(J)>0; (b) 1−Tr(J)+∑M×2(J)−Det(J)>0;

(c) 1−∑M×2(J)+Det(J)

[

Tr(J)+Det(J)

]

>0.

Conditions (a) and (b) correspond to relations that hold for any admissible combination of parameter values, while condition (c) requires the inequality

0

inequality, one gets:

 inequality in proposition 4.

A Neimark-Sacker bifurcation will occur when the following equality is observed:

[

( ) ( )

]

0 equivalent to the expression presented in proposition 4 respecting the bifurcation point.

Finally, if the system is not stable and we are not over a bifurcation point, then the system will be locally unstable, as referred through point c) of proposition 4

Proof of proposition 5: In the case n=3, one has realized that two of the eigenvalues of matrix J are positive while the other two are negative. This observation allows to compile a set of inequalities that if jointly satisfied imply that local stability holds. These conditions are the following:

i) (1+λ1)⋅(1+λ2)⋅(1+λ3)⋅(1+λ4)>0; first two conditions (i and ii).

The stability conditions may be transformed, after some calculus (that is particularly tedious for the third condition), into the following:

i) 1+Tr(J)+∑M×2(J)+Det(J)>0;

ii) 1−Tr(J)+∑M×2(J)−Det(J)>0;

The first two conditions hold under the system’s assumptions; condition iv) is true

for (1 )2

These are the conditions for stability; instability prevails if one of them is not fulfilled.

A Neimark-Sacker bifurcation requires once again the product of eigenvalues to be equal to one, that is, λ1⋅λ2 =1 or λ3⋅λ4 =1 (or both) 

Proof of proposition 6: It is straightforward to verify that the balanced growth path is unique and that it corresponds to the capital value in the proposition. For such, just solve the following equation in order to k ,

any equivalent relation. The notion of stability requires those eigenvalues to be above -1 and below 1. Thus, since the expression in the proposition corresponds to referred expression

Proof of proposition 8: Just note that the stability condition 1+Tr(J)+Det(J)>0 is always guaranteed; the left inequality in the proposition



 

θ − + −δ <ψ a

A

1 holds under 1-Det(J)>0 and the right inequality in the proposition



 

 ⋅

< + θ

ψ a

a

1 is satisfied for 1-Tr(J)+Det(J)>0, given the values of the trace and the determinant of the matrix in linearized system (8)

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Figures

Figure 1 – Local dynamics in the model without optimization (n=1).

Figure 2 – Local dynamics in the model without optimization (n=2).

Det(J)

)

2(J M×

Bifurcation point

+ +

+

+ 2

1 2 2 ) 2 1 (

2 µ

µ µ

+ +

+

2

1 2 2

2 µ 2 µ

Stability area

Det(J)=1 Det(J)

Tr(J)

1+Tr(J)+Det(J)=0 1-Tr(J)+Det(J)=0

1

Figure 3 – Bifurcation diagram (A, k~t

) for the model without optimization (n=1).

Figure 4 – Bifurcation diagram (A, k~t

) for the model without optimization.

A closer look, for 0.253<A<0.276 (n=1).

Figure 5 – Lyapunov exponents in the model without optimization (n=1).

Figure 6 – Attractor for the model without optimization (A=0.25; n=1).

Figure 7 – Attractor for the model without optimization (A=0.33; n=1).

Figure 8 – Basin of attraction for the model without optimization (A=0.33; n=1).

The area in black is the basin.

Figure 9 – Time series of k~t

for the model without optimization (A=0.25; n=1).

Figure 10 – Bifurcation diagram (A,k~t

) for the model without optimization (n=4).

Figure 11 – Local dynamics in the model with optimization (n=1).

Figure 12 – Local dynamics in the model with optimization, for a selected array of parameter values and a varying A (n=1).

1 1.049

Det(J)=1 Det(J)

Tr(J) A=0

2.791

A→+∞

1.628

Det(J)=1 Det(J)

Tr(J)

1+Tr(J)+Det(J)=0 1-Tr(J)+Det(J)=0

1

Figure 13 – Bifurcation diagram (A,k~t

) for the model with optimization (n=1).

Figure 14 – Attractor for the model with optimization (A=0.2593; n=1).

Figure 15 – Time series of k~t

for the model with optimization (A=0.2593; n=1).

Figure 16 – Basin of attraction for the model with optimization (A=0.2593; n=1).

The area in black is the basin.

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