A quotient space is a vector space obtained by identifying all vectors that differ by a vector in a fixed subspace. If is a subspace of , then the quotient space is written
It is read as “ modulo ” or “ by .” Informally, the construction collapses the whole subspace to zero and keeps track of what remains outside . More formally, its elements are equivalence classes, also called cosets, of the form .
27.1 The Basic Idea
Let be a vector space over a field , and let be a subspace.
Two vectors are regarded as equivalent modulo when their difference lies in :
This means that and are considered the same after we ignore all movement inside .
The quotient space is the set of all equivalence classes under this relation.
27.2 Cosets
The equivalence class of a vector is
This class is more commonly written as
Thus
The set is called a coset of in .
If , then
So every vector in belongs to the same coset as . In the quotient space, all vectors of become the zero element.
27.3 The Quotient Space
The quotient space is
Its elements are not individual vectors of . Its elements are cosets.
This distinction is important. A vector belongs to . A coset belongs to .
The zero vector of is
Thus the subspace itself becomes the zero element in the quotient.
27.4 Equality of Cosets
Two cosets are equal exactly when their representatives differ by an element of :
This gives the practical test for equality in a quotient space.
For example, if
and
then two vectors
belong to the same coset if their difference lies in . That means
This happens exactly when
So in , only the second coordinate remains relevant.
27.5 Operations on Cosets
Addition in the quotient space is defined by
Scalar multiplication is defined by
These definitions are natural: choose representatives, perform the operation in , then take the resulting coset.
The operations are well-defined because changing representatives by elements of does not change the final coset. This relies on being a subspace.
27.6 Well-Defined Addition
We must check that the definition of addition does not depend on the chosen representatives.
Suppose
and
Then
Since is closed under addition,
Therefore
So addition is well-defined.
27.7 Well-Defined Scalar Multiplication
Suppose
Then
For any scalar ,
because is closed under scalar multiplication.
Therefore
So scalar multiplication is well-defined.
27.8 Vector Space Structure
With the operations
and
the quotient is a vector space over .
Its zero element is
The additive inverse of is
Indeed,
The vector space axioms follow from the corresponding axioms in .
27.9 Geometric Picture in
Let
and let
Then is the -axis.
For a vector
the coset is
This is the horizontal line through height .
Thus can be viewed as the set of all horizontal lines. Each horizontal line is one element of the quotient space. Since only the height matters, this quotient is naturally isomorphic to .
27.10 Geometric Picture in
Let
and let
Then is the -plane.
For
the coset is
This is the horizontal plane at height .
Therefore can be identified with the remaining coordinate . Hence
The quotient collapses the entire -plane direction and keeps only the vertical direction.
27.11 Quotient by a Coordinate Subspace
Let
and let
Then consists of all vectors whose last coordinates are zero.
Two vectors in are equivalent modulo exactly when their last coordinates agree.
Thus
The quotient removes the first coordinate directions and preserves the remaining directions.
27.12 Dimension of a Quotient Space
If is finite-dimensional and is a subspace of , then
This number is called the codimension of in :
For example, if
and
then
The quotient keeps the directions not already accounted for by .
27.13 Proof of the Dimension Formula
Let
Choose a basis of :
Extend it to a basis of :
Then
We claim that
form a basis of .
First, they span . Any vector can be written as
In the quotient, the terms from vanish:
Second, they are linearly independent. If
then
So
for some scalars . This gives a linear relation among the basis vectors of . Hence all coefficients are zero, in particular
Therefore
27.14 The Quotient Map
There is a natural linear map
defined by
This is called the quotient map or canonical projection.
It is linear because
and
It is surjective because every element of has the form .
27.15 Kernel of the Quotient Map
The kernel of the quotient map
is exactly .
Indeed,
But
means
This holds exactly when
Therefore
So quotienting by is precisely the operation of making into the zero subspace.
27.16 Quotients and Linear Maps
Let
be a linear map.
If , then is constant on each coset of . That is, if
then
so
Therefore
This means descends to a well-defined map on the quotient:
given by
The quotient space is designed exactly to support this kind of construction.
27.17 First Isomorphism Theorem
Let
be a linear map. Then
The isomorphism is
defined by
This is well-defined, linear, one-to-one, and onto.
This theorem says that after collapsing exactly the vectors killed by , what remains is the image of .
27.18 Example: Projection onto One Coordinate
Define
by
The kernel is
the -axis.
The image is all of .
By the first isomorphism theorem,
This matches the geometric picture: quotienting by the -axis leaves only height.
27.19 Quotients and Direct Sums
Suppose
Then every vector can be written uniquely as
where
In the quotient ,
Thus every coset has a unique representative in . Therefore
So when splits as a direct sum, quotienting by leaves the complementary part .
27.20 Summary
A quotient space is formed by identifying vectors of that differ by an element of the subspace . Its elements are cosets . The whole subspace becomes the zero vector of the quotient.
The key ideas are:
| Concept | Meaning |
|---|---|
| Equivalence modulo | when |
| Coset | |
| Quotient space | Set of all cosets |
| Zero coset | |
| Quotient map | |
| Kernel of quotient map | |
| Dimension formula | |
| First isomorphism theorem |
Quotient spaces express the idea of ignoring a subspace. They appear whenever a linear construction identifies several vectors as equivalent and keeps only the information that remains after that identification.