Quotient space – Serlo

In this article we consider the quotient space of a -vector space with respect to a subspace . The quotient space is a vector space in which we can do computations as in , up to an addition of arbitrary terms from .

Introduction Bearbeiten

Computations with solutions of a linear system Bearbeiten

We consider the matrix

 

We now want to solve the linear system of equations   for different vectors  . For example, taking  , we get a solution   and for  , we get a solution  . That is,   and   hold. What is then the solution for  ? To find this out, we can use linearity of  : We just have to add our previous solutions together, since  . Thus, a solution to   is given by  .

The solution to the above system of equations is not unique. For instance, the system   is also solved by   and the system   is also solved by  . The solutions   and  , as well as   and   differ from each other. Their differences are   and  . Both   and   are solutions to the (homogeneous) linear system  . That is, they lie in the kernel of  .

To-Do:

Link kernel of a matrix

This "kernel property" is true in general: if   and   are two different solutions of  , they differ exactly by an element in the kernel of  , because  . Since the kernel of   is important, we give it the separate name   in the following. Conversely, whenever we have two solutions   and   of  , then their difference   is in the kernel  . So once a single solution is found, then the kernel can be used to find all solutions to the system. Put differently, we can consider two vectors whose difference is in   as equivalent, since if one vector solves  , then the other also does.

For scalar multiplication by  , we can use linearity of   again: We have a solution   of   and we want to solve   without recalculating. Again, we can obtain a solution by using our already determined solution  : We have  , so   is a solution to  . For the second solution   this also works:   is a solution of  . Again, the difference of both (equivalent) solutions   and   is in  . So we can scale solutions of linear systems to find solutions to scaled systems. While scaling, the differences stay in  , so both solutions stay equivalent. A different way to say that two vectors are equivalent is to say that they are the same modulo   whenever they differ only by some vector in  . For example, the solutions   and   of the system of equations   are equal modulo  , since  . When calculating with solutions of systems of linear equations, we therefore calculate modulo  .


Construction of the quotient space Bearbeiten

In the example, we made calculations in a vector space  , but only looked at the results up to differences in a subspace  . That is, we considered two vectors   and   in   as equivalent, whenever  . To formalise these "calculations up to some element in  ", we identify vectors which using an equivalence relation   that is defined by

 

This is exactly the relation we used to define cosets of a subspace. In this article, we have also checked that   is an equivalence relation. Mathematically, the set of all equivalence classes is denoted by  .

We will now show that on  , we can define a natural vector space structure. To do so, we introduce an addition   and a scalar multiplication   on  : For   and   we define

 

These definitions make use of representatives. That is, we took one element from each involved coset to define   and  . However, we still have to show that the definitions are independent of the chosen representative.

That is, we must show that this definition is independent of the choice of representative and thus makes sense. We give this proof further below. The property that a mathematical definition makes sense is also called well-definedness.

We also need to show that   is a vector space with this addition and scalar multiplication, which we will do below.

Definition Bearbeiten

In the previous section, we considered what a vector space   might look like, in which we can calculate modulo  . The elements of   are the cosets  . We want to define the vector space structure using the representatives. Further below , we then show that the definition makes mathematical sense, that is, the vector space structure is proven to be well--defined.

To distinguish addition and scalar multiplication on   from that on  , we refer to the operations on   as " " and " " in this article. Other articles and sources mostly use " " and " " for the vector space operations.

Definition (Quotient space)

Let   be a  -vector space and   be a subspace of   with

 

being the set of cosets of   in  . Further, let  .

We define the addition in   by:

 

Analogously, we define scalar multiplication on   as:

 

Explanation of the definition Bearbeiten

A short explanation concerning the brackets appearing in   and  : To define the addition   in  , we need two vectors from  . Vectors in   are cosets, so   and   denote cosets given by  . The expression   is also a coset, namely the one associated with  :

 

The scalar multiplication works similarly: For a scalar   and a coset   with   we want to define  . For this we first calculate the scalar product   in   and then turn to the associated coset  :

 

So we first execute the addition or scalar multiplication of the representatives in   and then turn to the coset to get the addition or scalar multiplication on  . Mathematically, we also say that the vector space structure on   "induces" the structure on  .

Well-defined operations in the quotient space Bearbeiten

We want to check whether the operations of   and   are independent of the choice of representatives - that is, they are well-defined.

Theorem (Well-defined operations in the quotient space)

Let   be a  -vector space and   a subspace of vectors. Then addition and scalar multiplication on   are well-defined.

Proof (Well-defined operations in the quotient space)

For well-definedness, we need to show the following: If in the definition, we plug in different representatives of the coset(s) on the left-hand side, we end up with the same coset on the right-hand side. Mathematically, we have to show :

  • For  : If   and  , then  .
  • For  : If   and  , then  .

Proof step: Well-defined addition

By definition of a coset we have to show that   holds. Since  , this is equivalent to  . Now   and   or   and   each represent the same coset modulo  . Thus,  . Since   is a subspace of  , it follows that  . So the addition   is indeed independent of the choice of representatives.

Proof step: Well-defined scalar multiplication

Well-definedness of the scalar multiplication   can be seen in same way: In the above notation, we have to show that  . Since   and   represent the same coset modulo  , we have  . And since   is a subspace, we also have  . So the scalar multiplication   is also independent of the choice of representative.

Establishing the vector space axioms Bearbeiten

We show that the quotient space is again a  -vector space by taking the axioms valid for   and inferring those axioms of  . Hence, taking quotient spaces is a way to generate new vector spaces from an existing  -vector space, just like taking subspaces.

Exercise (Proof of the vector space axioms in quotient space)

Let   be a  -vector space and   a subspace of it, then   with the operations   and   defined above is also a  -vector space

Solution (Proof of the vector space axioms in quotient space)

Proof step: Establishing properties of a commutative additive group (also called an Abelian group).

We first consider the properties of addition. For this let  .

1. Associativity:

We trace back the associativity to associativity in  

 


2. Commutativity

We also trace commutativity back to commutativity in  

 


3. Existence of a neutral element

Since we are considering displacements of  , the coset   should be the neutral element with respect to addition. We can verify this by using that   is the neutral element in  :

 

4. Existence of an inverse

We consider the coset  . For the inverse   of  , we need that

 

Thus, the addition of an element with its inverse indeed yields the neutral element  .

We also trace the inverse of   back to inverse in  . Let   be a representative of   and   its inverse in  . Then,

 

Thus, the element inverse to   is  .

Proof step: Distributive laws

1. Scalar Distributive Law

Multiplication of a vector (in a quotient space, i.e., the vector is a coset) with a sum of scalars yields:

 

2. Vector Distributive Law

Likewise, we can show that the distributive law also holds for the multiplication of a scalar with the sum of two vectors (i.e., with two cosets in the quotient space):

 

Proof step: Properties of scalar multiplication

We now show that the scalar multiplication of cosets also satisfies the corresponding vector space axioms. Again, we trace back properties in the quotient space back to the corresponding properties in  . To this end, let   and  . Then the following axioms hold:

1. Associative law for scalars

The scalar multiplication is associative, since

 


2. Neutral element of scalar multiplication

We want to prove that   is also the neutral element for  . That is,   must hold. Since 1 is neutral in   and since  , we get

 

So   is the neutral element of scalar multiplication and   is indeed a  -vector space.

Examples Bearbeiten

Satellite images Bearbeiten

Example (Satellite images)

 
Skyline of New York
 
Satellite image of New York

We imagine that we are standing on a vantage point in New York City from which we are looking at the skyline. In this situation, we will see the city in three dimensions. So objects (e.g. skyscrapers) can be identified with vectors in  . However, there are also situations where we want to look at the city in only two dimensions, for instance, when taking a virtual tour using a map or a satellite image of New York.

If we want to create a map or a satellite image, we need to "project" information from three dimensions into two dimensions. This process can mathematically be described by a reduction to some quotient space  .

For example, let us take a look at the edge of a skyscraper. On the oblique image, we see that an edge reaches about 600 feet up into the air. However, on the satellite image, the edge is just displayed as a dot. So all points (= vectors) on the edge are identified with this one dot. The dot is then a coset in  . The vector space   is given by the (1-dimensional)  -axis, since after adding a vector on the  -axis (i.e., shifting a point up or down), we end up at the same dot on the sattelite image. The space   contains all dots, i.e., it corresponds to the (2-dimensional) map.

Example in finite vector space Bearbeiten

Now, we turn to a more abstract mathematical example, that will involve some donuts.

Example (Quotient space in  )

In the vector space article, we considered the abstract mathematical set  , which can be seen as lattice points on a torus (= surface of a donut). Using the same method, we can think of   as 9 lattice points on a torus as well:

We obtain a torus from a square by stretching gluing the edges as follows:

 
Gluing a square to a torus
 
Forming a torus from a plane

In other words, the surface of a donut is the same as a square, where, if you walk out on one edge, you immediately enter it at the opposite side. Thus we may visualize   as follows: On the torus, we draw nine points in lattice form. We then get the following picture:

 
Visualization of a two-dimensional vector space over a field with three elements on a torus

The subspace   generated by  , corresponds to a discrete straight line. We put this line through the above points.

 
Visualization of a subspace in F3^2 on a torus

We now have points lying on two different sides directly next to our line. Some points are lying directly to the right of the line; that is, they are displaced from the straight line by  . Some other points lie directly to the left of our line; that is, they are displaced by  . In the picture it looks like this:

 
Visualization of the cosets of a subspace in F3^2 on a torus

The vector space   also allows for "adding the points on the donut": Here, we get the following relations:

  1. If we add a point on the left and a point on the right of the line, we get a point on the line: For example,  .
  2. If we add two points on the left of the line, we get a point on the right: For example, we have  .
  3. If we add two points on the right of the line, we get a point on the left: For example,  .

If we form the quotient space   (with 3 cosets), we see that two points have the same position with respect to the line (on/left/right) if they are in the same coset. Each coset then consists of 3 points. Furthermore, our addition relations above just represent the addition on the quotient space  .

Relationship between quotient space and complement Bearbeiten

In the quotient space   we calculate with vectors in   up to arbitrary modifications from  . We know another construction that can be interpreted similarly: The complement. A complement of a subspace   is a subspace   such that  . Here   denotes the inner direct sum of   and   in  , that is,   and  . A vector   can then be decomposed uniquely as  , where   and  . But the complement itself is then not unique! There can be different subspaces  , with  .

For the quotient space, we "forget" the part of   that is in   by identifying   with the coset  :

 

If   is a complement of   and   for distinct   and  , then we can analogously forget the  -part by mapping   to the  -part, called  :

 

Apparently   and the complement   are similar. Can we identify the two vector spaces   and  , i.e., are they isomorphic? Yes, they are, as we prove in the following theorem.

Theorem (Isomorphism between complement and quotient space)

Let   be a complement of   in  . Then the projection   is a linear isomorphism between   and the quotient space  .

Proof (Isomorphism between complement and quotient space)

We want to show that   is linear, i.e., compatible with addition and scalar multiplication, and bijective.

Proof step: Linearity of  

Since   is a subspace and scalar multiplication and addition is defined on representatives,   is compatible with addition and scalar multiplication. That is, for   and  , we have

 

and

 

Proof step: Surjectivity of  

Let  . Since   is a complement of  , we find   and   with  . Then

 

where we used in   that   and thus   holds. So   is surjective.

Proof step: Injectivity of  

We show  . Let  , i.e.   with  . So   holds. Thus  . Since   is a complement of  , we have  . Further,   and   implies  , so  .

We have seen that   is isomorphic to any complement of  . So it should also behave like a complement, i.e.   should hold. But be careful: Because   is not a subspace of  , we cannot form the inner direct sum with  . However, we can still consider the outer direct sum of   and  :

 

This may not be equal to  , but it may be isomorphic to  . And we will show that it indeed is isomorphic.

Theorem ( )

Let   be a subspace of a  -vector space  . Then,   holds.

Proof ( )

Let   be a complement of  , i.e.   and  . From the previous theorem we know that the function

 

is an isomorphism. We use this to show that

 

is an isomorphism, where   denotes the outer direct sum.

Proof step:   is linear

We have   for all  . It follows directly that   is linear, since addition and scalar multiplication on   are defined component-wise and as   and   are linear.

Proof step:   is bijective

This also follows from   for all  , since the identity   and   are bijective.

Thus we have  . By this theorem, the inner direct sum of the subspaces   and   is isomorphic to their outer direct sum. So  , where   denotes the inner direct sum of   and  .

To-Do:

link "this theorem" to the appropriate theorem

Exercises Bearbeiten

Exercise (The projection is linear)

Let   be a  -vector space and   a subspace. Show that the canonical projection.

 

is linear.

Solution (The projection is linear)

Let   and   be arbitrary. We again write   and   for the vector space structure on  . We then have

 

So   is linear.