As is well known, the theory of retractions is always one of interesting topics in Euclidian and Non-Euclidian space and it has been investigated from the various viewpoints by many branches of topology and differential geometry El-Ahmady [1].

El-Ahmady [1-13] studied the variation of the density function on chaotic spheres in chaotic space-like Minkowski space time, folding of fuzzy hypertori and their retractions, limits of fuzzy retractions of fuzzy hyperspheres and their foldings, fuzzy folding of fuzzy horocycle, fuzzy Lobachevskian space and its folding, the deformation retract and topological folding of Buchdahi space, retraction of chaotic Ricci space, a calculation of geodesics in chaotic flat space and its folding, fuzzy deformation retract of fuzzy horospheres, on fuzzy spheres in fuzzy Minkowski space, retractions of spatially curved Robertson-Walker space, a calculation of geodesics in flat Robertson-Walker space and its folding, and retraction of chaotic black hole.

An n-dimensional topological manifold M is a Hausdorff topological space with a countable basis for the topology which is locally homeomorphic to. If is a homeomorphism of onto, then h is called a chart of M and U is the associated chart domain. A collection () is said to be an atlas for M if. Given two charts such that, the transformation chart between open sets of is defined, and if all of these charts transformation are -mappings, then the manifolds under consideration is a -manifolds. A differentiable structure on M is a differentiable atlas and a differentiable manifolds is a topological manifolds with a differentiable structure Arkowitz [14] Banchoff [15], Dubrovin [16], Kuhnel [17], Montiel [18].

Most folding problems are attractive from a pure mathematical standpoint, for the beauty of the problems themselves. The folding problems have close connections to important industrial applications Linkage folding has applications in robotics and hydraulic tube bending. Paper folding has application in sheet-metal bending, packaging, and air-bag folding Demainel [19]. Following the great Soviet geometer Pogorelov [20], also, used folding to solve difficult problems related to shell structures in civil engineering and aero space design, namely buckling instability El Naschie [21]. Isometric folding between two Riemannian manifold may be characterized as maps that send piecewise geodesic segments to a piecewise geodesic segments of the same length ElAhmady [4]. For a topological folding the maps do not preserves lengths El-Ahmady [5,6].

A subset of a topological space is called a retract of if there exists a continuous map such that where is closed and is open El-Ahmady [3,7]. Also, let be a space and a subspace. A map such that for all is called a retraction of onto and is the called a retract of This can be re stated as follows. If is the inclusion map, then is a map such that If, in addition, we call r a deformation retract and a deformation retract of X Another simple-but extremely useful-idea is that of a retract. If then A is a retract of X if there is a commutative diagram.

If and then is a retract of g if there is a commutative diagram Arkowitz [14], Naber [22], Shick [23] and Strom [ 24].

The flat Robertson-Walker Line element is one example of a homogeneous isotropic cosmological spacetime geometry, but not the only one. The general RobertsonWalker Line element for a homogeneous isotropic universe has the form where dl² is the line element of a homogeneous, isotropic threedimensional space. There are only three possibilities for this. Let’s now look at the closed flat Robertson-Walker model. In the present work we give first some rigorous definitions of retractions, folding and deformation retraction as well as important theorems of closed flat Robertson-Walker model. In what follows, we would like to introduce the types of retraction, folding and deformation retraction of closed flat RobertsonWalker model El-Ahmady [11,12], Hartle [25], Straumann [26] with metric

The coordinate of closed flat Robertson-Walker space are

where the range of the three polar angles is given by and

Now, we use Lagrangian equations

To find a geodesic which is a subset of the closed flat Robertson-Walker space. Since

Then the Lagrangian equations for closed flat Robertson-Walker space are.

From Equation (5) we obtain constant say, if, we obtain the following cases:

If hence we get the coordinates of closed flat Robertson-Walker space which are given by

.

Which is the sphere, , it is a minimal geodesic and minimal retraction. Also, ifhence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the hypersphere, , it is a minimal geodesic and minimal retraction. Again, ifhence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the hypersphere, it is a minimal geodesic and minimal retraction. Also, ifhence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the hypersphere, , it is a minimal geodesic and minimal retraction. If hence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the hypersphere, , it is a minimal geodesic and minimal retraction. Again, if hence we get the coordinate of closed flat Robertson-Walker space which are given by

.

This is the sphere, it is a minimal geodesic and minimal retraction. Also, if hence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the hypersphere, , it is a minimal geodesic and minimal retraction. If hence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the sphere, , it is a minimal geodesic and minimal retraction. Again, ifhence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the hypersphere, it is a minimal geodesic and minimal retraction. Also, ifhence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the hypersphere, it is a minimal geodesic and minimal retraction. If hence we get the coordinate of closed flat RobertsonWalker space which are given by

Which is the hypersphere, it is a minimal geodesic and minimal retraction. Again, ifhence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the hypersphere, it is a minimal geodesic and minimal retraction. Also, if hence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the sphere, it is a minimal geodesic and minimal retraction. If hence we get the coordinate of closed flat RobertsonWalker space which are given by

This is the sphere, it is a minimal geodesic and minimal retraction. Again, if hence we get the coordinate of closed flat Robertson-Walker space which are given by

.

Which is the point of the hypersphere , it is a minimal geodesic and minimal retraction. Also, if hence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the sphere, it is a minimal geodesic and minimal retraction. If hence we get the coordinate of closed flat RobertsonWalker space which are given by

.

Which is the point of the hypersphere , it is a minimal geodesic and minimal retraction . Also, if hence we get the coordinate of closed flat Robertson-Walker space which are given by

Which is the sphere, it is a minimal geodesic and minimal retraction .

Theorem 1. The retractions of closed flat RobertsonWalker space are minimal geodesics and geodesic spheres.

In this position, we present some cases of deformation retract of open flat Robertson-Walker space. The deformation retract of open flat Robertson-Walker space is

where be the open flat Robertson-Walker space and is the closed interval [0, 1], be present as

The deformation retract of the open flat RobertsonWalker space into the sphere is

where

and

The deformation retract of the open flat RobertsonWalker space into the sphere is

The deformation retract of the open flat RobertsonWalker space into the sphere is

Now, we are going to discuss the folding of the open flat Robertson-Walker space Let, where

An isometric folding of the open flat RobertsonWalker space into itself may be defined by

The deformation retract of the folded open flat Robertson-Walker space into the folded geodesic is:

with

The deformation retract of the folded open flat Robertson-Walker space into the folded geodesic is:

The deformation retract of the folded open flat Robertson-Walker space into the folded geodesic is:

Then, the following theorem has been proved.

Theorem 2. Under the defined folding and any folding homeomorphic to this type of folding, the deformation retract of the folded open flat Robertson-Walker space into the folded geodesics is the same as the deformation retract of open flat Robertson-Walker space into the geodesics.

Now, let the folding be defined by:

where

The isometric folded open flat Robertson-Walker space is:

The deformation retract of the folded open flat Robertson-Walker space into the folded geodesic is:

with

The deformation retract of the folded open flat Robertson-Walker space into the folded geodesic is:

The deformation retract of the folded open flat Robertson-Walker space into the folded geodesic is:

Then, the following theorem has been proved.

Theorem 3. Under the defined folding and any folding homeomorphic to this type of folding, the deformation retract of the folded open flat Robertson-Walker space into the folded geodesics is different from the deformation retract of open flat Robertson-Walker space into the geodesics.

Lemma 1. The relations between the retractions and the limits of the folding of open flat Robertson-Walker space discussed from the following commutative diagrams

Lemma 2. The end of limits of the folding of closed flat Robertson-Walker space is a 0-dimensional space.

Proof. Let

Let

.

Consequently, -dimensional sphere, it is a minimal geodesic.

Lemma 3. The relation between the retraction and the deformation retract of open flat Robertson-Walker space discussed from the following commutative diagram

Theorem 4. Any folding of into induces folding of B into from

Proof. Let

, then there is an induced folding

such that

and

such that the following diagram is commutative

i.e.

Theorem 5. Any retraction of into

induces retraction of

into.

Proof. Let r be a retraction map,

where and are the open sphere in

. Also, let

and

such that.

Then we have the retraction such that

Theorem 6. Any retractionthen the map induced by the exponential map.

Proof. Let a retraction, be a retraction of into. Also, Let and.

Then we have the retraction

such that

Theorem 7. Any retraction, then the map induced by the inverse exponential map.

Proof. Let a retraction, be a retraction of int. Also, Let

and.

Then we have the retraction

such that

Theorem 8. If the retraction of the sphere is, the inclusion map of is, and inclusion map of is. Then there are induces retractions such that the following diagram is commutative.

Proof. Let the retraction map of the hypersphere is, the inclusion map of is , the retraction map of is, the retraction map ofis given by, and. Hence, the following diagram is commutative.

Theorem 9. If the retraction of the sphere is, and.

Then there are induces exponential inverse map such that the following diagram is commutative.

Proof. Let the retraction map of the hypersphere is,

,, , and. Hence, the following diagram is commutative.

The present article deals what we consider to be closed flat Robertson-Walker model. The retractions of closed flat Robertson-Walker model are presented. The deformation retract of closed flat Robertson-Walker model will be deduced. The connection between folding and deformation retract is achieved. New types of conditional folding are presented. Also, the relations between the limits of folding and retractions are discussed. Some commutative diagrams are presented.