A sensor records the position of a point in space but ignores its height. It cannot tell from , or from any other point on the vertical line through them. Is there a sensible way to treat each such line as one object, and then to add and scale these objects? The quotient space does exactly this, and the real work is checking that every answer is the same whichever point of a line we happen to pick.
Key terms
Equivalence modulo a subspace
Definition Let be a vector space over , where is or , and let be a subspace of . Two vectors are equivalent modulo , written , when
This is an equivalence relation. It is reflexive because , symmetric because and is closed under negatives, and transitive because and is closed under addition. No finite dimension and no inner product are needed.
In plain words Two vectors count as the same when they differ only by a vector of , the directions we have agreed to ignore.
Example In let be the vertical axis, spanned by . The difference lies in , so . In general two vectors are equivalent exactly when their first two coordinates agree. The subspace hypothesis matters. If the set in were used in place of a subspace, the condition would not even be reflexive, since is not in the set.
Coset
Definition For , the coset of modulo is the set
It is the equivalence class of , and is called a representative of it. Two cosets satisfy exactly when . If with , then , and runs over all of as does, so the two sets agree. Conversely, if the cosets are equal, then lies in , so for some and . Two cosets are either equal or disjoint, because a common point gives . So the cosets split into pieces that do not overlap. A coset is a subspace only when it contains , which happens exactly when and the coset is itself.
In plain words A coset is a copy of shifted so that it passes through . Every point on it is an equally good name for it.
Example With the vertical axis in , the coset is the vertical line . It equals , and it is not a subspace, since it misses the origin. The coset of any vector on the axis, such as , is the axis itself.
Quotient space
Definition The quotient space is the set of all cosets with , with the operations
for and . These rules are well defined, as the next key term shows, and with them is a vector space over the same field . Its zero vector is the coset , and the negative of is . Every other axiom follows by doing the matching calculation on representatives and taking the coset of the result.
In plain words The elements of are whole cosets, not vectors of . To add two cosets, add any representatives and take the coset of the sum.
Example In modulo the vertical axis,
Choosing the representatives at heights and instead gives . That is a different vector, but it lies on the same vertical line, so the resulting coset is the same. Likewise , which is the coset .
Well-defined operation
Definition A rule on is usually written with a representative, so it is a genuine function only if equivalent representatives always give the same result. For a function on , the rule is well defined exactly when, for all ,
For a rule with several inputs, every input may be replaced by an equivalent representative. Coset addition and scaling pass this test. If and with , then
so the sum and the scalar multiple land in the same cosets whichever representatives we use. Both checks use only that is a subspace.
In plain words A formula written with one representative must give an answer that all the other representatives agree with. Trying one or two choices is evidence, not proof, so the check has to cover every choice at once.
Example In modulo the vertical axis, the rule is well defined, because moving along a vertical line changes only . The rule is not. The vectors and name the same coset , yet the rule would assign it both and .
Quotient basis
Definition Let be finite-dimensional over and let be a subspace. Take a basis of and extend it to a basis of . Then the cosets form a basis of , called a quotient basis. They span, because any satisfies
the terms with falling into the zero coset. They are independent, because means , so for some scalars , and the independence of the extended basis forces every . When the extension is not unique, and different extensions can give different quotient bases.
In plain words The directions of become zero in the quotient. Only the added directions survive, and among them nothing is lost or repeated.
Example For and , extend by and . The cosets and form a quotient basis, and
Extending by and instead gives different representatives but the same cosets, since and .
Dimension of a quotient space
Definition If is finite-dimensional over and is a subspace of , then
This follows by counting the quotient basis above, which has members. In particular is the zero space exactly when , and has the same dimension as .
In plain words Each dimension of takes one dimension away from the quotient. Which directions survive depends on , so a quotient is not found by deleting an arbitrary coordinate.
Example In let , so . Since
every coset satisfies . The coset is not zero because , so it alone is a quotient basis. The cosets of and both have coordinate , and indeed they are equal, since . The vector could not represent a basis element, because its coset is the zero coset.
Check yourself
- In let . Which of the cosets and equals ?
Show the answer
Compare differences of representatives. The difference lies in , so . The difference is not a multiple of , so is a different coset.
- In let . Decide whether each rule is well defined on , first and then .
Show the answer
The first rule is not well defined. The vectors and represent the same coset , but the rule gives for one and for the other. The second rule is well defined. Any two representatives of one coset have the form and with , and . A single pair that happens to agree would not prove this, which is why the argument works with an arbitrary .
- In let . Find , a quotient basis, and the coordinates of in that basis.
Show the answer
The two spanning vectors are independent, so and . The matrix with columns , , and has determinant , so these four vectors form a basis of , and , is a quotient basis. For any vector,
so the coordinates of the coset are and . For they are and . As a check,