For the linear map , its image of a linear map and kernel of a linear map are
Both contain the zero vector, since . If and belong to the image of a linear map, then for any real numbers ,
Thus is a vector subspace of . If , then
so is a vector subspace of .
The rank of a linear map and nullity of a linear map are
The rank-nullity theorem states that
To prove it, choose a basis of the kernel of a linear map and use basis extension to obtain a basis
of . The vectors span the image of a linear map: applying to an arbitrary linear combination of the displayed basis removes all the terms. They are also linearly independent. Indeed,
so for some scalars . The linear independence of the extended basis forces every and to vanish. Consequently and , proving the identity. The same argument covers an empty basis when one of these dimensions is zero.
Here . By the rank-nullity theorem, , and a dimension is a nonnegative integer. All three possibilities occur:
The images of a linear map in these examples have dimensions , respectively, while the corresponding kernel of a linear map is , and . The identity above excludes all other pairs.
If , every would satisfy , so would be a surjective linear map. But its image of a linear map has dimension at most , whereas . Therefore no such exists. This is the obstruction to a right inverse: cannot reach every target vector.
The necessary and sufficient condition is
For necessity, if and , then .
For sufficiency, let be a basis of and suppose the kernel of a linear map is trivial. The vectors are linearly independent, since implies . Extend them to a basis of . Define a linear map by
Then agrees with the identity operator on a basis, hence on all of . Thus a left inverse exists precisely when is injective; this is the linear left inverse criterion.
An elementary row operation is one of three reversible changes: interchange two rows; multiply one row by a nonzero scalar; or add a scalar multiple of one row to a different row. Their inverses are, respectively, the same interchange, multiplication by the reciprocal, and addition of the negative scalar multiple.
Applied to an augmented matrix, these changes interchange linear equations, rescale an equation by a nonzero factor, or add a multiple of one equation to another. Every old solution satisfies the new equations. Applying the inverse elementary row operation gives the converse, so the solution set is unchanged at every step. Equivalently, all the operations together give
where is an invertible matrix, a product of elementary matrices.
Writing the unknown vector as , the first two linear equations give and . Substitution into the third gives
Thus, when , put . There is exactly one solution:
When , the remaining equation is . Hence
The second case is an affine line in a vector space, so it contains infinitely many solutions. These cases exhaust all real numbers .
A system of linear equations is solvable exactly when . If is one solution, then
so its solution set is , a translate of the kernel of a linear map.
For , the matrix is an invertible matrix, and
Every is in the image of a linear map and has exactly one preimage. For , its first two columns span the image of a linear map, while the corresponding homogeneous linear system gives the kernel of a linear map:
The prescribed satisfies the displayed condition precisely when . If , it lies outside the image of a linear map and there is no solution. If , it lies in the image of a linear map, and the nonzero kernel of a linear map supplies infinitely many solutions.
For , , whose row space is . For , elementary row operations give the reduced row echelon form
Its row space is , whereas the image of a linear map is . These differ: belongs to the former but not the latter. Thus (A) is true exactly when . Rows are being identified with vectors in in this comparison.
Every elementary column operation preserves the linear span of the columns: each new column is a linear combination of the old columns, and the inverse operation supplies the reverse inclusion. Thus the column space of equals that of , which is precisely the image of a linear map . Consequently (B) is true for every .
For , both reduced forms are , so . At , the reduced column echelon form is the transpose of the reduced row echelon form of , giving
For example, followed by , using the updated second column, produces the displayed directly. Its third column is zero. The two matrices differ, so (C) is true exactly when . Taking a transpose exchanges the kind of reduction, but also replaces the original by ; it does not generally identify the two reduced forms of itself.
Choose the rotation taking to , to and to itself. The columns of the matrix of a linear map are these images of the standard basis, so
This fixes the orientation used throughout this question.
Using the convention , the characteristic polynomial is
Since for every , the only eigenvalue over the real numbers is . Solving gives
Thus the only eigenspace over the real numbers is the axis of the rotation.
The two nonzero proper invariant subspaces are
Both are preserved by the rotation. To show there are no others, note that
is the linear projection onto , and is the linear projection onto . Every invariant subspace is preserved by , and hence by both of these linear projections. Therefore
Because has dimension one, is either or . If contains a nonzero , it also contains . These two vectors are linearly independent, because their two-dimensional determinant is . They span , so is either or . The only possibilities for are therefore .
Finally every has the unique decomposition , with one summand in each of . Hence
This also illustrates how invariant subspaces of a quarter-turn in three dimensions can be classified by linear projections.
Over the complex numbers, the characteristic polynomial splits into three distinct roots of a polynomial, . Direct multiplication gives the eigenvectors
They are linearly independent: the last two have two-dimensional determinant in the first two coordinates, and the first has nonzero third coordinate. Thus
This is a basis of eigenvectors of , proving that has a diagonalizable matrix.
The prescribed form is a sum of products of real polynomial evaluations. It is a symmetric bilinear form, since each evaluation is a linear map. Also
Equality forces . A nonzero polynomial of degree of a polynomial at most two cannot have three distinct roots of a polynomial, by the root bound for a polynomial. Thus equality holds only for the zero polynomial, establishing positive definiteness. Therefore the form is a real inner product, and is an inner product space. This is a discrete sampling inner product on polynomial spaces.
The relevant inner products are
Hence and are orthogonal vectors. Dividing by their norms gives the orthonormal basis
of their linear span .
For any orthonormal basis of , bilinearity gives
Together with , these identities prove pairwise orthogonality. The construction subtracts the orthogonal projection onto a finite-dimensional subspace from , leaving the orthogonal projection residual.
Use from i. Their inner products with are
Thus . Its values at are , so
By ii the three polynomials are orthogonal vectors, and normalizing gives
This orthonormal set is a basis of the three-dimensional vector space . It is the result of the Gram-Schmidt process applied to .
If is an orthogonal transformation and is an orthonormal basis, then
The images form an orthonormal set, hence are linearly independent and form an orthonormal basis in dimension three.
Conversely, suppose the images of one chosen orthonormal basis form an orthonormal basis. Write and . By linearity of and bilinearity,
Thus mapping one orthonormal basis to an orthonormal basis is equivalent to preserving every inner product. In the converse, a single chosen orthonormal basis suffices.
Put and use the orthonormal basis from iii. The columns of the given matrix give
Consequently
The images of are therefore , again an orthonormal basis. By i, is an orthogonal transformation. Its matrix in this orthonormal basis is
is not an orthogonal matrix. Its first column has squared Euclidean norm
so . The reason this is compatible with ii is that is not an orthonormal basis for the given inner product. Its Gram matrix is
The correct condition on this matrix representation of a linear map is
which follows either by direct multiplication or by the inner product preservation just proved. This is the rule for an orthogonal transformation in a nonorthonormal basis.
For a subgroup of , the left coset represented by is
Suppose two left cosets intersect. There are such that , so
Because is a subgroup, . Thus, for every , , proving . Interchanging the two representatives gives the reverse inclusion. Therefore two left cosets are equal or disjoint.
Lagrange's theorem states that if is a subgroup of a finite group , then
where the index of a subgroup is the number of distinct left cosets.
Every lies in , since . By i, distinct left cosets are disjoint, so these sets form a partition of a set . Each has cardinality : the function from to is a bijection, with inverse , by cancellation in a group. Counting the elements in this finite partition of a set gives , proving the theorem.
The order of a group element is the smallest positive integer with . Such an integer exists in a finite group: two powers in must agree, and cancellation gives a positive power equal to .
By minimality, are distinct. Every integer power of is one of them, by division of its exponent by . They form the cyclic subgroup
Applying Lagrange's theorem to this subgroup gives
For , the element belongs to both and . The assumed equal-or-disjoint property therefore gives .
If , then , so is closed under multiplication. Also , so some satisfies . Therefore . Along with the given identity element, closure and existence of inverse elements establish that is a subgroup of . This is the subgroup test. The proof even works without assuming that is finite.
Choose and put . Then . For any ,
so these translates are equal or disjoint by the assumed property of . Applying i shows that is a subgroup. Thus
This proves that is a left coset. Together with i, it gives the equal-or-disjoint translates characterize cosets criterion.
Let , with a prime number, and choose . By Lagrange's theorem, the order of a group element divides and is greater than one. It is therefore , and . Hence a group of prime cardinality is a cyclic group.
The converse is false: the cyclic group has four elements, and is not a prime number.
If , any two elements are , and
Thus every cyclic group is an abelian group.
For the converse, the Klein four-group is an abelian group, with componentwise multiplication. Each nonidentity element has order of a group element two, so none generates its four elements. It is therefore not a cyclic group.
The hypothesis implies for every , including . For ,
Thus is an abelian group. This is the group of exponent two is abelian argument.
The converse is false: the cyclic group is an abelian group, but its two nonidentity elements have order of a group element three.
Choose distinct , possible because . By iii, and commute, and . The four elements
are distinct: would give , while or would make or . Commutativity and show that products stay in , and every element is its own inverse. More explicitly,
is a group isomorphism, with addition of exponents modulo two. Hence contains a subgroup isomorphic to the Klein four-group.
The converse is false. The direct product of groups contains , but it has elements of order of a group element three. Thus the existence of the specified subgroup does not force every nonidentity element to have order of a group element two.
The complete classification up to group isomorphism is
Here is the trivial group. The prime number cases follow from i. For four elements, an element of order of a group element four generates . If there is none, Lagrange's theorem makes every nonidentity element have order of a group element two. Then iv produces a four-element subgroup, which must be all of , giving the Klein four-group.
For six elements, an element of order of a group element six gives . Suppose there is none. If there were no element of order of a group element three either, all nonidentity elements would have order of a group element two. Part iv would then produce a subgroup of cardinality four, contradicting Lagrange's theorem. Thus choose of order of a group element three. There is also an involution : otherwise the five nonidentity elements could be paired into distinct pairs , impossible for an odd number of elements.
The subgroup has index of a subgroup two, so it is a normal subgroup. Indeed, for , both and are the complement of , and for both equal . Consequently is either or . The first possibility makes commute, and then has order of a group element six: forces , so both and divide . This contradicts our assumption. Therefore
Every element is uniquely or , with , and the relation determines all their products. Sending to and to gives a group isomorphism with the symmetric group . This completes the classification of groups of order at most six.
Of these groups, exactly embed in . Concrete subgroups are
There is no subgroup, since does not divide . There is no subgroup either: the order of a group element in a symmetric group is the least common multiple of the lengths in its disjoint cycle decomposition, and on four letters the only possibilities are .
Label the vertices of a regular tetrahedron , and include all its Euclidean isometries, both rotations and reflections. The following list describes every subgroup of cardinality at most six, allowing arbitrary relabelling of the vertices. The numbers count actual subgroups, rather than just their group isomorphism types.
Here is why this is exhaustive. Part b leaves only the trivial group, . The disjoint cycle decomposition gives exactly the two listed kinds of involutions, the three-cycles, and the four-cycles, accounting for all the cyclic subgroups. In a Klein four-group, the nonidentity elements commute. If it contains , any other nonidentity element must be a commuting involution, hence or ; either choice yields the displayed opposite-edge subgroup. If it has no transposition, its three nonidentity elements must be all three double transpositions, yielding the rotational subgroup.
Finally, an subgroup has a unique cyclic subgroup of cardinality three. Its two three-cycles fix the same unique vertex. Every element of the subgroup preserves this vertex, since conjugation preserves that unique cyclic subgroup. Thus it is the full stabilizer subgroup of that vertex. The counts in the list are consequently exhaustive, giving
The two kinds of and the two kinds of Klein four-groups have different geometric behavior despite having the same abstract group isomorphism type within each pair. This is the distinction recorded by the small subgroups of tetrahedral symmetry.
A left group action of on a set is a function , written , satisfying
for all , . The orbit of a group action through and the stabilizer subgroup of are, respectively,
The identity element belongs to . If , then , so . If , applying to gives , so . These facts prove that the stabilizer subgroup is a subgroup of .
The orbit-stabilizer theorem identifies the orbit of a group action of with the set of left cosets of . Explicitly, there is a bijection
Here denotes a set of cosets; it is not asserted to be a quotient group. To prove the identification, observe that
This equivalence proves both well-definedness and injectivity. Every element of the orbit of a group action has the form , proving surjectivity.
In particular, for a finite group, the cardinalities satisfy
The last equality follows from Lagrange's theorem applied to the stabilizer subgroup.
The orbits of a group action form a partition of a set : every element lies in its own orbit of a group action, and two intersecting orbits of a group action coincide because each point can be moved back and then forward using inverse elements. By the orbit-stabilizer theorem, each orbit of a group action has cardinality dividing , so its size is or .
If every orbit of a group action had size or , their sizes would add to an even number, contrary to . Therefore there is a one-element orbit of a group action, say . Every sends into this same singleton, so
Thus is a fixed point of a group action. In fact the number of fixed points of a group action is odd, since all other orbits of a group action have even cardinality.
For a free group action, every stabilizer subgroup is . By the orbit-stabilizer theorem, every orbit of a group action has cardinality . Hence the two free group actions have the same number
of orbits of a group action. Choose one representative from each orbit of a group action and one representative from each orbit of a group action, and match them using .
Every has a unique expression . The orbit of a group action determines , and the free group action property determines : if , then , forcing . Therefore the rule
defines a function without ambiguity. For ,
which proves the required identity for every .
Indeed, is a bijection: its inverse is , well defined because the second is also a free group action. If is empty, the unique empty function already satisfies the identity. Thus the result holds in every case, and proves the stronger statement that free finite actions with equal cardinality are isomorphic.
Original solutions to all seven questions and all 42 lettered or Roman subparts of the ordinary sitting on 24 June 2015.
Call a peak of a sequence when for every . If there are infinitely many peaks of a sequence, list their indices in increasing order, . Since ,
This is a decreasing subsequence; throughout this argument, a decreasing monotone sequence may have equal successive terms.
If there are only finitely many peaks of a sequence, choose beyond all their indices; take if there are none. Every fails to be a peak of a sequence, so some satisfies . Starting with , choose such an recursively. This gives
The two cases prove the monotone subsequence theorem without any boundedness hypothesis.
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