For the stated angular-frequency Fourier transform convention, the convolution theorem givesThe Fourier inversion theorem and the assumed absolute integrability therefore imply
The Fourier transform of a derivative givesSince ,An arbitrary additive constant in affects only the zero-frequency Dirac delta function when transforms are interpreted as distributions.
For ,Multiplying on the left by and on the right by shows that it is equivalent to . Taking inverses gives . Thus is unitary exactly when is a normal matrix.
If is differentiable at and at , then is differentiable at andWrite , where , and put . Division by and passage to the limit proves the formula.
No. Take , , and . The function is not differentiable at , but is differentiable. Neither function is constant on an interval.
No. TakeBoth functions are nonconstant on every interval and nondifferentiable at zero, but is differentiable.
The comparison test says that if eventually and converges, then converges. If converges, its terms are bounded: . For ,so comparison with a geometric series proves absolute convergence.
The radius is the number for which the power series converges absolutely for and diverges for . Given , both and converge, so their terms are bounded, say . ThenThus ; letting gives .
This is the affine plane through , provided and are independent. The scalars are affine coordinates in those two directions.
The cross product of the plane normals is proportional to , soThe point on the intersection perpendicular to iswhich satisfies both plane equations and . Hence the line is .
The signed displacement of the sphere centre from the plane is . Orthogonal projection gives the circle centrePythagoras givesA real circle exists when : equality gives tangency and radius zero, while strict inequality gives a genuine circle.
The characteristic polynomial isFor , the eigenspace is spanned only by , so its geometric multiplicity is one although its algebraic multiplicity is two. Hence is not diagonalisable.
If , thenso the characteristic polynomials, eigenvalues, and algebraic multiplicities agree. The converse is false: and have the same characteristic polynomial, but the first is diagonalisable and the second is not, so they cannot be similar.
The Cayley-Hamilton theorem states that a square matrix satisfies its characteristic polynomial. If a matrix is diagonalisable, ; applying to the diagonal matrix gives zero and hence .
If , every eigenvalue satisfies , so all eigenvalues are zero and the characteristic polynomial is . Cayley--Hamilton then gives .
Choose an orthonormal eigenbasis of and set , . Part (a) shows that the form an orthonormal eigenbasis of . If and have these vectors as columns, then they are unitary andThis is the singular value decomposition.
Herewith eigenvalues and corresponding normalized vectors and . A compatible choice isDirect multiplication gives .
A real matrix is orthogonal when . If , norm preservation gives . If and , preservation of the Hermitian inner product gives ; distinct unit-modulus eigenvalues therefore have orthogonal eigenvectors.
The nonreal eigenvalues of a real matrix occur in conjugate pairs. Since their product is one and , the remaining real eigenvalue is . If , then , and , so : the plane is invariant.
The restriction to is a planar orthogonal map whose determinant is , hence a rotation through some . In an orthonormal basis adapted to ,Therefore and
The arithmetic--geometric mean inequality gives from onward. For ,so the tail decreases to a limit . Passing to the recurrence gives , hence .
For the subadditive sequence, , so it is bounded. The Fekete lemma can be proved directly here as follows. Let . Fix and write , . ThenThus , while the definition gives . Hence .
The alternating-series test says that implies convergence of . The hypothesis implies eventually, so is eventually decreasing. For some , eventually ; the divergent product of these factors forces . The test now applies.
The intermediate value theorem says that a continuous takes every value between and . For , the closed sets where and cannot separate the connected interval; equivalently, taking the supremum of and using continuity gives a point with value .
Set and for . Every interval contains a zero ; continuity on makes take every value between and , yet is discontinuous at .
A monotone function can be discontinuous only by a jump. If it had a jump at , any number strictly between the left and right limits would lie between and but would not be attained, contrary to the hypothesis. Thus it is continuous.
For the last assertion, pass to subsequences with both within of and near , near . For , the intermediate value theorem on the interval joining and gives with ; then . The endpoint cases use the original sequences.
The mean value theorem says that for continuous on , differentiable inside, for some . Applied to on ,which gives .
The ordinary mean value theorem gives for some . More generally, applying it to the difference of two translated functions shows inductively thatfor some . Taking proves the result.
No. The Darboux theorem says that every derivative has the intermediate-value property. Choose . In a deleted neighborhood of , the assumed limit puts within of . Darboux's theorem applied between and any such would require values near , which that neighborhood excludes. This contradiction shows that cannot be a derivative.
For a bounded function, the lower and upper integrals are the supremum of lower Darboux sums and infimum of upper Darboux sums. It is Riemann integrable when these agree.
Here for , so . On it has only finitely many discontinuities and is piecewise continuous, hence integrable. On its upper-minus-lower contribution is at most . Taking proves integrability on .
Changing variables givesThe average of a continuous function over tends to as . The two terms therefore tend to and , proving the stated limit.
The continuous approximation of a Riemann-integrable function follows here by choosing partitions with upper-minus-lower sum below . On each subinterval choose the midpoint of the infimum and supremum to form a step function . ThenReplace each of the finitely many jumps of by a linear transition on intervals of sufficiently small total length, obtaining a continuous with . Hence , and uniformly for every subinterval ,
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