Source: Mathematics Part A release, member FOI-20210708-1 - Data/4307.pdf, dated 17 June 2013. All 22 source leaf parts are answered below.
The department's solution-release policy excludes ordinary odd years; bounded exact-paper checks found no matching advertisement of full or selected worked answers. No parts are skipped.
The six question bodies coincide exactly with questions 1–6 of paper 4301; their solutions are reused verbatim while retaining this paper's distinct cover identity and section tree.
The dual space is the vector space of all linear functionals on :
Addition and scalar multiplication are defined pointwise. The annihilator of a vector subspace is
It is a vector subspace of : linear combinations of functionals vanishing on also vanish on .
Choose a basis of . Because , the list is linearly independent. Extend it to a basis of . A linear functional is specified uniquely by its values on a basis, so define to be zero on the and on every added basis vector other than , and set .
Then vanishes on every linear combination of the , so , while
This proves that the annihilator of a vector subspace separates every vector outside the subspace from that subspace; no inner product or preferred coordinates are needed.
Every vanishes on , so . Conversely, suppose . Every is a linear combination , giving . If , part (b) supplies a functional in with , a contradiction. Therefore
For the dimension statement, take a basis of and extend it to a basis of . Relative to the corresponding dual basis, a functional belongs to precisely when its first coefficients are zero. Thus
If , this says and the empty intersection is understood to be .
In the coordinate example choose the linear functionals and . Their kernels are the two coordinate planes
Their intersection is the stated axis, and .
The adjoint operator is characterized by
This identity works with either convention for which argument of the complex inner product is linear, provided the convention is used consistently.
For uniqueness, subtract the two given identities to get for every . Fix and choose . Then positive definiteness gives
so . As was arbitrary, . The decisive fact is that a vector orthogonal to every vector, including itself, must be zero.
First suppose . For , choose with . For ,
Thus . The direct sum of vector spaces gives , while the orthogonal complement has . Equal finite dimensions imply .
Conversely, suppose . Decompose arbitrary vectors as and , with and . Since is the indicated projection, and . Orthogonality makes the cross terms vanish, so
Therefore satisfies the defining identity of its own adjoint operator. By uniqueness from part (a), . Hence
This is the characterization of an orthogonal projection among projections along a complementary subspace.
A Euclidean domain is an integral domain admitting a Euclidean function such that division with a smaller remainder is possible: for every and nonzero , there are with
Thus the Euclidean function measures progress in repeated division. Definitions which additionally normalize it to be nondecreasing under multiplication give the same class of Euclidean domains; the division property is the one needed below.
For the zero ideal, choose . Otherwise choose a nonzero for which the Euclidean function is minimal; the well-ordering principle guarantees such a choice. For any , perform Euclidean division:
Because is an ideal, . A nonzero remainder would contradict the minimal choice of , so and . Thus . Conversely, implies , proving
Every ideal is therefore a principal ideal; in particular, a Euclidean domain is a principal ideal domain.
For the Gaussian integers, use the Gaussian norm
To identify the ideal, note that is even if and only if have the same parity. Also
This quotient is a Gaussian integer precisely when have the same parity. Therefore the prescribed set consists exactly of the multiples of , giving
Any associate of would generate the same principal ideal.
Under the assumed continuous real differentiability, the necessary and sufficient conditions are the Cauchy-Riemann equations at every point of :
Necessity follows by computing the complex derivative along real and imaginary increments. For sufficiency, real differentiability gives the first-order expansion
The Cauchy-Riemann equations turn the linear part into , so the complex derivative exists and equals . Thus is a holomorphic function on .
At any , take sufficiently small so . The complex difference quotient is
Hence the complex derivative exists at every point of the punctured plane, and
The excluded point is essential to the domain statement: the reciprocal has a simple pole there.
Write . Both moduli are nonnegative, so squaring preserves their strict inequality:
Thus
The boundary is the perpendicular bisector of and in the complex plane; the strict inequality selects the half-plane containing .
Use the reciprocal Möbius transformation
It is a holomorphic function on by part (b). For ,
Part (c) now gives if and only if , so . Conversely, because . For any , put ; the same identity gives , so and . Finally, reciprocation is injective on nonzero complex numbers. This proves bijectivity, with inverse
The inverse is also holomorphic, so this is a biholomorphism.
For a piecewise continuously differentiable contour , the contour integral is defined by
If the contour has corners, integrate on its finitely many differentiable pieces and sum the results. The integral on the right is taken componentwise as an ordinary real-parameter integral of a complex-valued function. The factor encodes both the speed and orientation of the contour.
Choose the continuous argument with values in and define
Its branch cut is the nonpositive imaginary axis, including zero, exactly the removed ray. Locally away from that ray, the Cauchy-Riemann equations or the local inverse of the exponential show that it is a holomorphic logarithm, with derivative and . The chosen interval fixes the additive ambiguity by integer multiples of .
Use the branch from part (b) and close the real interval with the upper semicircle, oriented counterclockwise. For , the number has positive imaginary part, so the numerator is a holomorphic logarithm throughout a neighbourhood of the contour and its interior. The branch point lies strictly below the contour. The only enclosed pole of
is the simple pole at , with residue
To justify discarding the arc, take . On it, lies between and , and the argument has bounded absolute value. Hence
The real-axis integral is absolutely convergent, since its integrand is at infinity and has no real singularities. The residue theorem therefore gives
Finally, . Taking twice the real part yields
The branch choice affects the first integral's imaginary part; the second integral is real and independent of that choice.
An isolated singularity at means that is holomorphic in some punctured disk , while itself is an excluded point or a point where the given function is not holomorphic. There are no other singularities arbitrarily close to . By Laurent's theorem, the function has a unique Laurent series on that punctured disk:
The negative-power terms form its principal part of a Laurent series.
A removable singularity is an isolated singularity for which the function on the punctured disk extends to a holomorphic function on the full disk, by assigning or correcting its value at . In Laurent series terms,
The remaining power series defines the extension with value at . Conversely, a holomorphic extension has a Taylor series there, so uniqueness of the Laurent series forces all negative coefficients to vanish.
A pole of order at has finitely many negative powers in its Laurent series, the lowest being exactly :
Equivalently,
Thus has a holomorphic extension with nonzero value at , whereas multiplying by any smaller power does not remove the singularity.
A zero of order at means that is holomorphic near and
Equivalently its Taylor series starts with the nonzero coefficient of , so
Unlike a pole, a zero is a regular point of the function itself; its reciprocal has a pole of the corresponding order.
By the finite-order zero factorizations,
with holomorphic near . Shrinking the disk if necessary, continuity ensures never vanishes there, so is holomorphic and nonzero at . Consequently
If , the exponent is , with a holomorphic nonvanishing factor. Hence
With the same factors, if , then
has no negative power and extends holomorphically across . Thus its apparent singularity is a removable singularity, with extension value
For the extended quotient has a zero of order ; for the extension is nonzero.
The complex sine has simple zeros exactly at , , because and . Hence the denominator has a zero of order three at each of these points and nowhere else.
At , the numerator has order two, so the quotient has a simple pole. Indeed its leading term is . At , the numerator has order one, so there is a pole of order two. At , the numerator has order three, cancelling the denominator's order-three zero, so the singularity is removable. Its extension value is
At every remaining , the numerator is nonzero, giving a pole of order three. Thus the complete finite-plane classification is
Away from this discrete set the denominator is nonzero, so the quotient is holomorphic.

Articles by others on the same topic (0)

There are currently no matching articles.