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1G (Number Theory)

Words: 265 Articles: 6

a

Words: 84 Articles: 1

Solution

Words: 84
The binomial theorem gives
The central binomial coefficient is the largest of these nonnegative binomial coefficients, so
For the upper bound, fix a prime number . By Legendre formula,
Each summand is either zero or one. Hence the P-adic valuation satisfies
If , this implies
There are at most such prime numbers. If instead , then , so the P-adic valuation is at most one. Multiplying the prime-power contributions therefore yields
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b

Words: 74 Articles: 1

Solution

Words: 74
Write the Chebyshev theta function as
Taking natural logarithms in part a gives
and hence
Because , the right-hand side is at least for every sufficiently large integer .
Now let be sufficiently large and set using the floor function. Then and , so the monotonicity of gives
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c

Words: 107 Articles: 1

Solution

Words: 107
Suppose that the positive integer is a decisive number. For every prime number , the composite number satisfies . It therefore cannot be coprime to , so .
The product of all prime numbers below consequently divides . Taking natural logarithms gives
Changing the strict endpoint can remove at most one prime term. By part b, for every sufficiently large the right-hand side is at least, for example, . This is impossible for sufficiently large , since
Thus every decisive number lies below one fixed bound, and only finitely many integers can do so.
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2F (Topics In Analysis)

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i

Words: 115 Articles: 1

Solution

Words: 115
The polynomial form of Runge theorem says that if is compact, is connected, and is holomorphic on a neighbourhood of , then for every there is a polynomial such that
Statement (i) is false. Take the entire function . It is bounded on the closed first quadrant . If polynomials converged uniformly to on , then each sufficiently late would be bounded on the positive real axis. A polynomial bounded on that ray must be constant. No sequence of constants converges uniformly to on , since its values at zero and near infinity differ by one.
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ii

Words: 52 Articles: 1

Solution

Words: 52
Statement (ii) is true. Let
Each is compact and has connected complement. By the polynomial Runge theorem, choose a polynomial with
Every fixed belongs to for all sufficiently large , so . Thus the convergence is pointwise on .
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iii

Words: 81 Articles: 1

Solution

Words: 81
Statement (iii) is false. Let be a thin open annulus about the unit circle, let , and split the circle into two proper closed arcs whose union is the whole circle. Each arc has connected complement, so polynomial approximation of the reciprocal on a proper circular arc gives uniform polynomial approximations to on each separately.
If polynomials converged uniformly to on , then uniform convergence on the unit circle and the Cauchy integral theorem would give
a contradiction.
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iv

Words: 42 Articles: 1

Solution

Words: 42
Statement (iv) is true. Apply the Weierstrass approximation theorem separately to the real and imaginary parts of the continuous function on the compact interval . Combining the two real polynomial sequences gives complex polynomials converging uniformly to on .
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3I (Coding and Cryptography)

Words: 200 Articles: 1

Solution

Words: 200
Write for the all-one column vector. The parity-check extension of a linear code is
The defining map is linear, so is a binary linear code. If is a generator matrix and a parity-check matrix for , then one may take
The punctured code in, say, the last coordinate is
Coordinate deletion is a linear map, so is linear. Its generator matrix is obtained by deleting the last column of . If the minimum distance is at least two, deletion is injective on , and hence has the same dimension as .
For its parity-check matrix, first use invertible row operations on to make its nonzero last column a coordinate vector. The last column is nonzero because otherwise the weight-one word supported there would belong to , contrary to . Delete the pivot row and the last column; the resulting matrix is a parity-check matrix for . Equivalently, is obtained by shortening the dual code at the deleted coordinate.
Finally, the shortened code in the last coordinate is
It is linear whenever is linear, because it is the puncture of the subspace .
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4I (Automata & Formal Languages)

Words: 321 Articles: 13

a

Words: 26 Articles: 1

Solution

Words: 26
For the formal grammar ,
Thus contains exactly the finite terminal words reachable from the start symbol by a finite grammar derivation.
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b

Words: 19 Articles: 1

Solution

Words: 19
Two formal grammars over the same terminal alphabet are equivalent when they generate the same language:
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c

Words: 46 Articles: 1

Solution

Words: 46
Two formal grammars over the same terminal alphabet are isomorphic when there is a bijection between their nonterminals such that and
where is extended to words by fixing each terminal and acting symbol by symbol.
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d

Words: 230 Articles: 6

i

Words: 58 Articles: 1
Solution
Words: 58
The grammars are isomorphic. The bijection
maps every production of to the corresponding production of . They are therefore equivalent. Notice that in the first grammar and in the second are unreachable; the isomorphism also preserves this irrelevant component.
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ii

Words: 90 Articles: 1
Solution
Words: 90
The grammars are non-equivalent. In the first grammar, terminal derivations without give
After applying any number of times while and remain adjacent, the production also gives
Hence, in particular, and .
In the second grammar, the fixed terminals in prevent and from ever becoming adjacent, so can never be used. The remaining productions give exactly
Thus , proving that the generated languages differ.
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iii

Words: 82 Articles: 1
Solution
Words: 82
The first grammar generates
because adds two 's and terminates the derivation.
In the second grammar, is a nonproductive nonterminal: every right-hand side of a -production still contains a . Consequently the branch never yields a terminal word. Every terminal derivation from instead uses repeatedly and ends with , so
The grammars are therefore equivalent, although they are not isomorphic.
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5J (Statistical Modelling)

Words: 92 Articles: 1

Solution

Words: 92
A one-parameter exponential family with natural statistic has density or probability mass function
where is the natural parameter of an exponential family and is the cumulant function of an exponential family. Its mean parameter is
The exponential-family deviance from to is twice the Kullback-Leibler divergence:
The carrier cancels from the likelihood ratio, so, with ,
For the Poisson distribution with mean ,
Therefore
Writing and applying the Taylor series of gives
so the second-order approximation is
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6C (Mathematical Biology)

Words: 201 Articles: 1

Solution

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With , the equilibria satisfy
Besides , the two positive equilibria are
where . Since
the nonzero equilibrium relation gives
The fixed point stability for an autonomous differential equation therefore shows that and are stable, while is unstable. The graph of starts at zero with negative slope, crosses upward at , crosses downward at , and tends to as .
For a constant input , write the equilibrium equation as
The low stable equilibrium and the intervening unstable equilibrium coalesce in a saddle-node bifurcation. More precisely, let be the first positive solution of
and define
Equivalently, and , with on the low-concentration branch. If , that branch no longer exists. Holding the input long enough carries the trajectory into the basin of attraction of the high state. When the input returns to zero, the concentration converges to
This is the saturating autocatalytic switch.
For , the threshold occurs at , so
The approximate double-root conditions are
Thus and
Hence the constant in is , as recorded by the strong-autocatalysis switching threshold.
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7E (Further Complex Methods)

Words: 199 Articles: 1

Solution

Words: 199
For
a finite point is an ordinary point exactly when and are holomorphic there. It is a regular singular point exactly when
are holomorphic at .
Put and . Direct differentiation gives
so the transformed equation is
Consequently is ordinary precisely when
are holomorphic at . It is a regular singular point at infinity precisely when and are holomorphic functions of near infinity.
If zero and infinity are regular singular and every nonzero finite point is ordinary, the Laurent series of and can contain only the terms compatible with both endpoint bounds. Hence
for constants . The equation is a Cauchy-Euler differential equation. Its indicial equation is
For distinct roots , the general solution on a domain with a chosen logarithm branch is
For a repeated root , the general solution of an Euler-Cauchy equation is
Finally require infinity to be ordinary. In the transformed equation its coefficients become
Both are holomorphic at zero exactly when and . Thus the further restriction is
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8D (Classical Dynamics)

Words: 152 Articles: 6

a

Words: 36 Articles: 1

Solution

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For smooth functions on the six-dimensional phase space with canonical coordinates , the Poisson bracket is
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b

Words: 40 Articles: 1

Solution

Words: 40
Hamilton's equations and the multivariable chain rule give
Thus the Hamiltonian conservation law gives
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c

Words: 76 Articles: 1

Solution

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For the phase-space dilation generator ,
Therefore the condition is the first-order equation
If for every positive real , differentiate with respect to at . The chain rule gives exactly
so every smooth scale-invariant satisfies the constraint. The same conclusion for negative follows wherever the stated invariance is defined; differentiation only needs the positive component containing .
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9B (Cosmology)

Words: 135 Articles: 1

Solution

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In the nonrelativistic regime,
The assumption puts the Fermi-Dirac distribution in its Maxwell-Boltzmann limit, so
Therefore the nonrelativistic Maxwell--Boltzmann number density is
For , chemical equilibrium and the vanishing photon chemical potential imply
Applying the number-density formula to each massive species and eliminating the chemical potentials gives
Use charge neutrality, , the mass approximation , and the convention in the question that suppresses the order-one internal-degeneracy ratio . With the Hydrogen binding energy
we obtain the Saha ionization equation
The assumptions are thermal equilibrium and chemical equilibrium before cosmological recombination, a nonrelativistic nondegenerate gas, zero photon chemical potential, charge neutrality, negligible proton-electron mass correction in the translational prefactor, and the stated degeneracy-factor approximation.
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a

Words: 18 Articles: 1

Solution

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For coprime integers with , the multiplicative order of modulo is
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b

Words: 56 Articles: 1

Solution

Words: 56
The Fermat-Euler theorem gives
so the multiplicative order exists. For every integer ,
Thus the modular exponential is periodic with period . If were a smaller period, then would give , contradicting the minimality of . Hence is its least positive period.
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c

Words: 27 Articles: 1

Solution

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Modulo ,
so . This order is even and
The factor extraction from an even modular order therefore gives
Thus
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d

Words: 49 Articles: 1

Solution

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The quantum Fourier transform measurement supplies a rational approximation
where is the desired multiplicative order. Here
Its reduced continued fraction convergent has denominator two, so continued-fraction recovery in quantum order finding proposes . Direct order verification from divisors confirms it:
Hence
As a check, the classical final step of the Shor algorithm gives
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11G (Number Theory)

Words: 326 Articles: 1

Solution

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Write an integral binary quadratic form as
A positive definite form is a reduced positive definite binary quadratic form when
with on the boundary or . The class number of a negative discriminant is the number of proper equivalence classes of primitive positive definite integral forms of discriminant .
Every such class has a reduced representative. For a reduced form,
so
There are only finitely many possible integers and , and then
is determined. Hence . There is at least one class: the principal form is
and
Thus , in agreement with the enumeration of reduced binary quadratic forms.
Now let be prime. The two forms
are primitive, positive definite, reduced, and have discriminant . They are not properly equivalent: represents one, while the least positive value of is two. Therefore
Assume henceforth that , so these are the only two classes. If
for a prime , then is odd and
Moreover , so is a quadratic residue modulo . This proves the necessity.
Conversely, suppose and is a quadratic residue modulo . By quadratic reciprocity, these two conditions imply
Indeed, for both relevant signs are positive, while for the signs from and reciprocity with cancel. Choose an even integer such that
Then
is a primitive positive definite integral form of discriminant and represents . It belongs to one of the two classes .
The second form cannot represent such a prime. If
then is odd and, since ,
This contradicts . Hence lies in the principal class , and proper equivalence of binary quadratic forms preserves represented integers. Therefore
This is the prime representation when h of minus eight q equals two.
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12I (Automata & Formal Languages)

Words: 324 Articles: 8

i

Words: 31 Articles: 1

Solution

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Extend to
by
The extended transition function of a deterministic finite automaton processes a whole word from left to right. The language accepted by is
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ii

Words: 57 Articles: 1

Solution

Words: 57
Let . The pumping lemma for regular languages states that every with can be written
with
Thus one may take the pumping number to be exactly the number of states of the given automaton, whether or not all of them are accessible.
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iii

Words: 77 Articles: 1

Solution

Words: 77
For , consider the ten prefixes
If , append
Then
because , whereas
Indeed, in a word ending in one , the prefix before the final positive run of 's must have length at most ten. Hence every pair is distinguished by some suffix. They occupy ten distinct Myhill-Nerode equivalence classes, so the minimal deterministic finite automaton for has at least ten states.
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iv

Words: 159 Articles: 1

Solution

Words: 159
Suppose first that is a regular language, accepted by a deterministic finite automaton . If two words reach the same state, then every continuation is accepted from both or rejected from both. Thus they are equivalent under , and the number of equivalence classes is at most the finite number of states of .
Conversely, suppose has finitely many classes. Define a deterministic automaton by
and
The transition is well defined: if , then for every suffix ,
so . Likewise, membership in is independent of the representative by taking the empty suffix in the definition of . Induction gives
so the automaton accepts exactly . It has finitely many states, and therefore is regular. This proves the Myhill-Nerode theorem in the stated formulation. The assumption merely says that the initial state is not accepting.
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13C (Mathematical Biology)

Words: 113 Articles: 6

a

Words: 29 Articles: 1

Solution

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Setting makes the inhibitor equation quasistatic:
Taking the spatial Fourier transform and using the Fourier transform of a derivative gives
Therefore the fast-inhibitor elimination in a reaction-diffusion system is
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b

Words: 35 Articles: 1

Solution

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Since and , the linearization is
For a spatial Fourier mode of the perturbation, part a gives
Thus with the dispersion relation after fast-inhibitor elimination
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c

Words: 49 Articles: 1

Solution

Words: 49
Put . At the threshold of a Turing instability, the maximum of
touches zero. Hence
The second equation gives . Substitution in the first gives
Therefore
and
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14B (Cosmology)

Words: 209 Articles: 6

a

Words: 44 Articles: 1

Solution

Words: 44
During matter domination,
The perturbation equation becomes
Substitution of the power law gives
whose roots are and . Hence the cosmic-time matter density modes give
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b

Words: 65 Articles: 1

Solution

Words: 65
Normalize and put . The cosmological horizon crossing condition is
For , matter domination gives , and therefore
For , radiation domination and continuity at equality give
Substitution in the crossing condition yields
These are the two branches of the horizon-crossing time across matter-radiation equality.
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c

Words: 100 Articles: 1

Solution

Words: 100
Neglect the decaying mode from part a. A mode that enters during matter domination grows in amplitude by
so its variance grows by . For , part b gives
For , the mode enters during radiation domination and is assumed not to grow significantly until equality. It then grows by . Since the equality mode satisfies
the post-equality variance growth is
Therefore the broken matter power spectrum from horizon entry is
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a

Words: 71 Articles: 1

Solution

Words: 71
Apply the gates from left to right. The first Hadamard gate and the first controlled-NOT gate produce the Bell state
The parallel gates then produce
The final controlled-NOT has the lower qubit as control; it interchanges and , whose amplitudes here are equal. Thus the output is
By quantum measurement in the computational basis, every basis outcome has probability equal to the squared modulus of its amplitude:
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b

Words: 83 Articles: 1

Solution

Words: 83
Use the inverse quantum circuit rule. Every gate in is self-inverse, so reverse their order. From left to right, the circuit for is:
1. a controlled-NOT with the lower qubit controlling the upper;
2. on the upper qubit and on the lower qubit;
3. a controlled-NOT with the upper qubit controlling the lower;
4. on the upper qubit.
This is the requested circuit description, with the two wires and control directions unchanged under each individual gate's adjoint.
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c

Words: 41 Articles: 1

Solution

Words: 41
Use three controlled-NOT gates with control-target directions
On computational-basis bits they act as
They therefore implement the Three-CNOT decomposition of the SWAP gate, and linearity proves the identity on every two-qubit state.
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d

Words: 72 Articles: 1

Solution

Words: 72
After the first Hadamard gate and the controlled unitary gate, the state is
The final Hadamard gate gives
Hence the Hadamard test returns one with probability
If , then and the outcome is zero with certainty. If , then modulo and the outcome is one with certainty. The single measurement therefore distinguishes the two promised cases exactly.
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16H (Logic and Set Theory)

Words: 501 Articles: 11

a

Words: 128 Articles: 1

Solution

Words: 128
Fix a set and define by recursion on
The recursion theorem defines a function-class uniquely by : for each there is exactly one finite sequence satisfying the displayed recursion through stage . Thus is genuinely functional, and the Axiom schema of replacement applied to the set gives the set .
Now define
It contains every member of . If , then for some ; hence every belongs to
Thus is transitive. If is any transitive set containing every member of , induction gives for every , so . Therefore
is the transitive closure of .
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b

Words: 168 Articles: 1

Solution

Words: 168
The Axiom of foundation says that every nonempty set contains an with . The principle of epsilon induction says that if a formula is progressive,
then holds for every set.
Assume foundation and let be progressive. If failed for some , use separation to form the nonempty set of failures inside . Foundation supplies an -minimal failure . Every member of lies in the transitive closure and is not a failure, so progressiveness gives , a contradiction. Hence epsilon induction holds.
Conversely, assume epsilon induction and suppose a nonempty set has no -minimal member. Let
If every member of satisfies but , then , making an -minimal member of , contrary to the assumption. Thus is progressive. Epsilon induction says every set lies outside , contradicting that is nonempty. Foundation follows.
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c

Words: 205 Articles: 6

i

Words: 75 Articles: 1
Solution
Words: 75
True. If is countable, then each of its members is a subset of this transitive set and is therefore countable.
Conversely, if is reasonable, then itself and every set occurring at every finite membership depth below it are countable. Starting with the countable set , each next level is a countable union of countable sets, hence countable. Their countable union is , so the transitive closure is countable.
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ii

Words: 53 Articles: 1
Solution
Words: 53
True. By part (i), the reasonable sets are exactly the hereditarily countable sets . The rank of a countable transitive closure is the supremum of countably many countable ordinals, plus at most a finite amount, and is therefore below . Hence every reasonable set belongs to
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iii

Words: 77 Articles: 1
Solution
Words: 77
False. The reasonable sets form the transitive set , but this structure fails the Axiom of power set. The set is reasonable, and every subset of is itself countable and therefore reasonable. Its full power set is uncountable, so it is not reasonable. No member of can therefore contain internally every subset of that belongs to . Thus the reasonable sets do not form a model of ZFC.
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17H (Graph Theory)

Words: 424 Articles: 8

a

Words: 113 Articles: 1

Solution

Words: 113
We prove the Quadratic Turan edge bound by induction. The case is immediate. For , if contains no , the induction hypothesis for gives the stronger bound. Otherwise choose a copy of . Every vertex outside has at most neighbours in , since one adjacent to all of would complete a . Thus the number of edges having at least one endpoint in is at most
The graph is still -free, so induction on the number of vertices gives
This proves the stated form of Turan theorem.
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b

Words: 120 Articles: 1

Solution

Words: 120
Let
be a longest path in . Every neighbour of either endpoint lies on . Suppose . Among the possible cut positions of the path, the sets
have total size greater than , so they intersect. The corresponding two edges close a cycle containing all vertices of .
If , connectivity supplies an edge from a vertex outside this cycle to a vertex on it. Breaking the cycle there and adjoining the outside vertex creates a path longer than , a contradiction. Hence
Since and , the long path from minimum degree gives . Thus contains .
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c

Words: 58 Articles: 1

Solution

Words: 58
Colour the vertices of in groups of size . Colour edges within groups blue and edges between groups red. The red graph is complete -partite, so it has no red . Every blue component has only vertices, so it has no path of length . Therefore
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d

Words: 133 Articles: 1

Solution

Words: 133
We first derive the Erdos-Gallai path edge bound from part b. If an -vertex graph has no path of length , then
Induct on , component by component. A component with at most vertices satisfies the bound trivially. A larger connected component cannot have minimum degree at least by part b, so delete a vertex of degree less than and apply induction; the integer degree removed is at most , which preserves the bound.
Now set
and consider a red-blue colouring of . If there is no red , part a with gives
Consequently
The path edge bound forces a blue . Together with part c this proves the clique-path Ramsey number
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18I (Galois Theory)

Words: 553 Articles: 10

a

Words: 86 Articles: 1

Solution

Words: 86
Let be a finite subgroup of and let be its exponent of a finite group. A finite abelian group contains an element whose order is its exponent: combine elements of maximal prime-power order across the primary components. Hence .
Every satisfies , so all elements are roots in the field of the nonzero polynomial . The Lagrange root bound over a field gives . Therefore , and the element of order generates . This proves that a finite subgroup of a field multiplicative group is cyclic.
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b

Words: 102 Articles: 1

Solution

Words: 102
A primitive root of unity is an th root of unity of multiplicative order exactly .
Let be primitive and let be the finite subgroup of that they generate. By part a, is cyclic. Its order is divisible by both and , hence by . On the other hand every element of has th power one, so the order of the cyclic group divides . Its order is therefore exactly , and a generator of is a primitive th root of unity in .
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c

Words: 102 Articles: 1

Solution

Words: 102
The cyclotomic polynomial is
where is primitive. Partitioning all th roots by exact order gives the cyclotomic factorization
Induct on . The quotient of the monic integer polynomial by the product of the already constructed monic , , lies in and is monic. Gauss lemma then shows that this quotient lies in .
If the prime does not divide , then over ,
Thus has no repeated root. Every factor, including the reduction of , is square-free, proving the Separability of a cyclotomic polynomial modulo p.
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d

Words: 132 Articles: 1

Solution

Words: 132
Choose a primitive root . Since every root of is a power of , its splitting field is . Each sends to another primitive root, uniquely of the form
The assignment is a homomorphism. It is injective because an automorphism fixing fixes .
If is irreducible over , the orbit of has all primitive roots, so the injection has image of size and is surjective. Conversely, surjectivity makes every primitive root a conjugate of . Its minimal polynomial over then has at least roots and divides the degree- polynomial , so it equals . This proves the Galois embedding for a cyclotomic polynomial and the claimed equivalence.
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e

Words: 131 Articles: 1

Solution

Words: 131
Let . We use the standard cyclotomic containment lemma: every root of unity in has order dividing . One proof uses the conductor of a rational cyclotomic field. The conductor attached to a primitive th root is , except that it is when ; containment in forces this conductor to divide , which gives .
If is even, , and the powers of already give all possible roots of unity in . If is odd, has order , so contains all th roots of unity, and the containment lemma shows there are no others. Thus the roots of unity in a rational cyclotomic field number
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19H (Representation Theory)

Words: 276 Articles: 4

a

Words: 153 Articles: 1

Solution

Words: 153
The Burnside lemma states that for a finite group acting on a finite set ,
To prove it, count
Counting by gives . Counting by gives
using the orbit-stabilizer theorem on each orbit . Dividing by proves the formula.
Let be the character of the permutation representation . Then , and a second application of Burnside's lemma gives
For a two-transitive action there are exactly two orbits on : the diagonal and the ordered pairs of distinct points. Hence . Transitivity says the trivial representation occurs once. Since the squared multiplicities of the irreducible constituents sum to two, there is exactly one further constituent, with multiplicity one, and it is irreducible and nontrivial. Thus
as in the permutation representation of a two-transitive action.
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b

Words: 123 Articles: 1

Solution

Words: 123
For permutation characters, Burnside lemma on a product gives
Two pairs and lie in the same -orbit exactly when
When , every value is possible because . Therefore the symmetric-group subset permutation representation satisfies
For , the inclusion map between subset permutation modules embeds into , so
is a character. Its norm is
By character orthogonality, is the character of an irreducible representation.
For , complementation is an -equivariant bijection , so
Consequently
the negative of one of the irreducible characters just found, and is not itself the character of a representation.
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20G (Algebraic Topology)

Words: 260 Articles: 1

Solution

Words: 260
Write a point of the band as with , , after rescaling the radius of the first three coordinates. The antipodal identification is
The homotopy is equivariant under this identification, so it descends to a deformation retraction of onto the central slice
Thus
The two boundary spheres of are exchanged by the antipodal map, so . This is the mapping-cylinder model of punctured real projective three-space.
The standard cellular chain complex for , with one cell in each dimension zero through three, has boundary maps alternating between multiplication by two and zero:
Therefore the integral homology of real projective three-space is
In particular,
Apply the Mayer-Vietoris theorem to
The relevant pieces of the long exact sequence are
and
The last map is injective, so
Since is simply connected and , the Seifert-van Kampen theorem gives
the infinite dihedral group. Topologically, is the double of punctured real projective three-space, namely .
The universal cover of each copy of is with two disjoint open balls removed, homeomorphic to . The universal cover of the double strings infinitely many such cylinders together according to the Cayley line of . Hence the familiar covering space is
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21F (Linear Analysis)

Words: 286 Articles: 6

a

Words: 153 Articles: 1

Solution

Words: 153
The Tietze extension theorem states: if is a normal topological space, is closed, and is continuous, then there is a continuous with .
We first prove an approximation lemma. Given continuous , the closed subsets
are disjoint and closed in . By the Urysohn lemma, there is a continuous equal to on and on . Then
Starting with and , apply the lemma recursively to obtain continuous such that
where . The series
converges uniformly by the Weierstrass test, so its sum is continuous. On , its remainder after terms is , which tends uniformly to zero; hence . The bounds also keep in after the standard endpoint-preserving version of the construction, proving the theorem.
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b

Words: 75 Articles: 1

Solution

Words: 75
Write
with each open. The closed sets and are disjoint. By the Urysohn lemma, choose a continuous with
The uniformly convergent series
defines a continuous map to . It vanishes on . If , then for some , so and . Thus
which is the closed G-delta set as a zero set construction.
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c

Words: 58 Articles: 1

Solution

Words: 58
Apply part b separately to obtain continuous with
Because , the two functions never vanish simultaneously. Hence
is continuous and takes values in . It equals zero exactly where , namely on , and equals one exactly where , namely on .
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22F (Analysis of Functions)

Words: 308 Articles: 6

a

Words: 93 Articles: 1

Solution

Words: 93
A weak solution is a function satisfying
The zero boundary condition is encoded by membership in .
On the Hilbert space define
The form is bounded and coercive:
The functional is bounded by the Cauchy-Schwarz inequality. The Lax-Milgram theorem therefore gives a unique weak solution and a bound
Thus is bounded. Composing it with the compact Rellich-Kondrashov compactness theorem for H01 embedding
shows that is the compact massive-Laplacian resolvent.
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b

Words: 118 Articles: 1

Solution

Words: 118
Extend and by zero outside the bounded set . Weak convergence makes bounded in . For each fixed ,
because .
Fix . On the finite-measure ball , the Fourier transforms are uniformly bounded by
Dominated convergence therefore gives
On the complementary region,
whose integral tends to zero uniformly in as by hypothesis. Splitting first at large and then taking , the Plancherel theorem yields
This is the same low-frequency compactness mechanism used in the Fourier proof of Rellich compactness.
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c

Words: 97 Articles: 1

Solution

Words: 97
Taking the Fourier transform of the distributional equation gives
because is even. The multiplier therefore gives the regularity gain for one plus an even power of the Laplacian
The Sobolev embedding theorem in its derivative form says that
To make all derivatives through order continuous, and simultaneously make continuous, it is enough and in general necessary to have
Under this condition the distributional identity is a pointwise identity, so is a classical solution. Thus
At the borderline , the standard Sobolev embedding does not in general give continuity.
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23F (Riemann Surfaces)

Words: 329 Articles: 1

Solution

Words: 329
The uniformization theorem states that every simply connected Riemann surface is conformally equivalent to exactly one of the Riemann sphere , the complex plane , or the open unit disc . Equivalently, every connected Riemann surface is a quotient of one of these by a free properly discontinuous group of conformal automorphisms.
For , every nonidentity Möbius transformation has a fixed point. A free action is therefore trivial, so the only surface uniformized by the sphere is
Every conformal automorphism of has the form . If , it has a fixed point, so a group acting freely consists only of translations. A discrete subgroup of has rank zero, one, or two. The corresponding quotients are
where is a rank-two lattice and is a complex torus. This proves the completeness of the Riemann surfaces uniformized by the complex plane.
Now let be a domain whose complement contains two distinct points. Its universal cover cannot be the sphere because no nonconstant holomorphic map from a compact Riemann surface has image in the noncompact proper domain . If its universal cover were , the covering map followed by would be a nonconstant entire function omitting the two chosen complementary points, contradicting the Little Picard theorem. The uniformization theorem therefore leaves only
which is the plane domain with two omitted points is hyperbolic result.
Finally let be a holomorphic embedding with compact. At each puncture zero and infinity, an essential singularity would, by the Great Picard theorem in a coordinate chart, force values to be taken repeatedly and contradict injectivity. Thus extends holomorphically to
A generic point of the open image has exactly one preimage, so has degree one. A degree-one holomorphic map between compact Riemann surfaces is a biholomorphism; equivalently, the Riemann-Hurwitz formula rules out branching and gives the same conclusion. Therefore the compact Riemann surface containing an embedded punctured plane is
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24G (Algebraic Geometry)

Words: 437 Articles: 1

Solution

Words: 437
For an algebraically closed field , the strong Hilbert Nullstellensatz says that every ideal satisfies
Its weak form says that exactly when . Now let and let be a homogeneous ideal. The affine zero set of is the affine cone over together with the origin. Hence, when the projective zero set is empty, either
or the affine zero set is exactly the origin. In the latter case the Hilbert Nullstellensatz gives
the irrelevant ideal of projective space. Equivalently, some power is contained in . These are precisely the alternatives in the Projective Nullstellensatz.
Let be a smooth quadric surface. After a projective linear transformation, the Segre embedding identifies
Choose distinct points . The two fibres
are the promised disjoint curves on a smooth quadric surface: each is a smooth projective line, and . By the Bézout theorem, any two nonempty curves in the projective plane intersect. An isomorphism of algebraic varieties preserves intersections and takes projective curves to projective curves, so these disjoint curves prove
Next let be a smooth projective curve and let be a rational map to a projective variety. At a point outside its initial domain, write
using elements of the function field . The local ring of a smooth algebraic curve at is a discrete valuation ring. If , multiplying every coordinate by a function of valuation makes all coordinates regular at and at least one a unit there. They therefore define a morphism near . Repeating this at the finitely many missing points proves the extension of a rational map from a smooth projective curve.
Smoothness is essential. Let be the normalization of a nodal curve for a rational nodal cubic . The inverse is a rational map on the smooth locus. If it extended to a morphism , then would agree with the identity on a dense Zariski-open subset of and hence everywhere. But the two distinct points above the node would satisfy
a contradiction. This is the failure of rational-map extension on a singular curve.
Finally take the Fermat cubic curve
and define the projective hypersurface
Because and have no common irreducible factor, the bihomogeneous polynomial is irreducible, so is an algebraic variety. Let
be the second coordinate projection. Every homogeneous cubic in three variables has a projective zero over , so every fibre is nonempty and is a surjective morphism. Over the fibre is the Fermat cubic curve, which is smooth and has genus
Over the fibre is
the union of exactly three distinct projective lines, hence exactly three irreducible components. This is the cubic pencil with a triangular member required by the question.
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25G (Differential Geometry)

Words: 533 Articles: 6

a

Words: 103 Articles: 1

Solution

Words: 103
Choose the orientation of a surface represented by a smooth Gauss map . The shape operator at is
If its principal curvatures are , then by definition
Let be a proper Euclidean motion of Euclidean three-space, so . Orient by transporting the normal:
The chain rule gives the orthogonal conjugacy
The determinant and trace are invariant under similarity, so the Euclidean invariance of the shape operator yields
If the surface orientation is reversed, then and are multiplied by . Therefore the orientation reversal of surface curvature says
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b

Words: 219 Articles: 1

Solution

Words: 219
A plane has both principal curvatures zero, hence . A circular cylinder of radius has principal curvatures and , hence
Because the absolute value of mean curvature is preserved even if one reverses the chosen orientation, no Euclidean motion can carry any open piece of the cylinder to an open piece of the plane. Thus the condition does not characterize planar pieces.
There are analogous examples for both signs of constant Gaussian curvature. Start with the arc-length surface of revolution
On a sufficiently small interval about , this is a regular surface and the curvatures of an arc-length surface of revolution give
At its mean curvature is
For this is a piece of the unit sphere and , whereas for it equals . By continuity, sufficiently small pieces around their central circles have disjoint ranges of , so no pieces in those chosen neighbourhoods are related by a Euclidean motion.
For curvature minus one, use
again on a sufficiently small interval. Then
The choices and give and . Restricting to small enough pieces again separates the ranges of . The constant Gaussian curvature surfaces of revolution therefore supply the requested noncongruent examples for and .
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c

Words: 211 Articles: 1

Solution

Words: 211
At , the surface cannot cross the boundary , because it lies inside . Consequently the two surfaces are tangent at . Apply a proper Euclidean motion of Euclidean three-space so that , their common tangent plane is , and the prescribed inward unit normal is . Locally write
with the region on the side . Then
Thus has a local minimum at zero and its Hessian matrix is positive semidefinite. The fundamental forms of a graph surface at a horizontal tangent plane give
Taking the trace of the positive-semidefinite difference proves the mean-curvature comparison at tangential contact:
There is no analogous conclusion for . In the same local coordinates take
Then , so the second graph lies on the inward side of the first, while the Gaussian curvature of a graph surface gives
Hence the mean-curvature inequality holds but
Using smooth bump functions, these local graph patches can be completed away from to a compact region with connected smooth boundary and a closed interior surface without changing their germs at . This realizes the counterexample under the global hypotheses.
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26K (Probability and Measure)

Words: 309 Articles: 6

a

Words: 111 Articles: 1

Solution

Words: 111
Let be a measure-preserving transformation of and let . The Birkhoff ergodic theorem states that
almost everywhere, where is the invariant sigma-algebra. The limit is -invariant and
Assume now that . For , let
be the bounded truncation of , and let be its Birkhoff limit. Since on a finite measure space, the dominated convergence theorem gives
Measure preservation and the triangle inequality give the contraction
Moreover, the almost-everywhere convergence and Fatou lemma imply
Consequently
Since in , letting proves the L1 convergence in the Birkhoff ergodic theorem on a finite measure space:
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b

Words: 60 Articles: 1

Solution

Words: 60
Let with irrational . This irrational rotation of the circle preserves Lebesgue measure and is ergodic. Apply the Birkhoff ergodic theorem to the indicator function . Its limit
is invariant, hence almost everywhere constant by ergodicity. Its integral must equal that of , so the constant is . Therefore
for Lebesgue measure-almost every .
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c

Words: 138 Articles: 1

Solution

Words: 138
Write the interval as , where , to avoid confusing its left endpoint with the rotation parameter . For every sufficiently large integer , define an inner and outer interval on the circle by
Apply part (b) simultaneously to this countable collection of intervals. The intersection of the corresponding full-measure sets still has full Lebesgue measure, and is therefore dense in the circle.
Fix an arbitrary . For each sufficiently large , choose with circle distance less than from . An irrational circle rotation preserves this distance, so for every ,
Averaging and using part (b) for gives
Letting proves the everywhere interval frequency under an irrational rotation:
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27J (Applied Probability)

Words: 443 Articles: 6

a

Words: 143 Articles: 1

Solution

Words: 143
In Kendall notation, the first two letters mean Poisson arrivals and exponential service times. An M-M-1 queue has arrival rate , one server of rate , and queue-length transitions
It has a stationary distribution of an M-M-1 queue exactly when
and then
An M-M-infinity queue has infinitely many servers, so every customer begins service immediately. Its occupancy transitions are
The detailed balance for a birth-death process equations give
Thus for every the stationary distribution of an M-M-infinity queue exists and is
the Poisson distribution of mean . The Burke theorem for an M-M-infinity queue states that in this stationary regime the departure process is a Poisson process of rate ; equivalently, time reversal turns departures into arrivals. The past departure process is also independent of the number in the system at the observation time.
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b

Words: 157 Articles: 1

Solution

Words: 157
Let be the number of telephone lines in use. The memorylessness of the exponential distribution makes a continuous-time Markov chain, specifically the M-M-infinity queue with generator rates
Suppose and put . Each initial call is still active at time with the exponential survival probability , independently of the others. Their surviving number is therefore
A call arriving at time survives until with probability . By Poisson thinning, the number of surviving new calls is independent of and has law
Hence in distribution. Multiplying the probability generating functions of the two independent random variables gives, for ,
Equivalently, the transient distribution of an M-M-infinity queue is
with independent summands. As , the binomial term converges to zero and the Poisson mean tends to . Therefore
which proves the stated large-time approximation.
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c

Words: 143 Articles: 1

Solution

Words: 143
For an M-M-1 queue, the first service lasts on average . During it, the mean number of arrivals is , and each arrival initiates another statistically identical busy-period family. Thus, when ,
so the mean busy period of an M-M-1 queue is
For the busy period is almost surely finite but has infinite mean, while for it is infinite with positive probability; in either case its expectation is infinite.
For an M-M-infinity queue, stationary occupancy is Poisson with mean , so the long-run probability of an empty system is
The process alternates between idle periods and busy periods. An idle period waits for the next Poisson arrival, so its mean is . The renewal-reward theorem, with reward equal to time spent empty, gives
Solving yields the mean busy period of an M-M-infinity queue:
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28K (Principles of Statistics)

Words: 441 Articles: 6

a

Words: 101 Articles: 1

Solution

Words: 101
Let be the multivariate normal density of . Under zero-one loss, the Bayes classifier chooses the class with the larger posterior probability. Thus
Equivalently, it chooses class one when the log posterior odds
is nonnegative. The decision boundary is .
If , the terms cancel, leaving
an affine function. This is the linear boundary of linear discriminant analysis. If , the quadratic part is
which is nonzero, so the boundary is a possibly degenerate quadratic hypersurface, as in quadratic discriminant analysis. This is the Gaussian Bayes classifier.
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b

Words: 154 Articles: 1

Solution

Words: 154
Condition on the observed value . If a classifier reports class zero, its conditional probability of error is ; if it reports class one, the conditional error is . Therefore the smaller conditional error is attained by class one exactly when
and by class zero exactly when the reverse strict inequality holds. Integrating these pointwise conditional errors proves that is a Bayes classifier.
The only possible nonuniqueness lies on the tie set
Because the two Gaussian class distributions are distinct, is not identically zero. It is a nonzero polynomial of degree at most two, so its zero set has Lebesgue measure zero. Both Gaussian laws have densities with respect to Lebesgue measure, hence assign probability zero to . Every Bayes rule must therefore agree with almost surely. This proves the uniqueness of a Bayes classifier up to the standard null-set equivalence of decision rules.
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c

Words: 186 Articles: 1

Solution

Words: 186
For , let be the Bayes classifier with class-zero prior , and define its two class-conditional error probabilities by
Writing the likelihood ratio as , the rule chooses class one when
The Gaussian likelihood-ratio level sets have probability zero, so dominated convergence shows that and depend continuously on . As , the threshold tends to zero and the classifier chooses class one almost surely, giving
As , it chooses class zero almost surely, giving the opposite limit . The intermediate value theorem therefore provides such that
The rule is an equalizer rule with worst-case risk . For any classifier ,
because minimizes the integrated risk for its prior. Hence is a minimax decision rule, as summarized by the minimax Gaussian Bayes classifier from equal class errors.
The prior is indeed least favorable. Its Bayes risk is , while for any other prior the Bayes risk is at most the integrated risk of the same equalizer rule , namely
Thus no prior has larger Bayes risk.
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29K (Stochastic Financial Models)

Words: 407 Articles: 8

a

Words: 78 Articles: 1

Solution

Words: 78
For every finite collection of positive times, is a linear transformation of the corresponding values of , so is a centered Gaussian process. If , then
Thus has the covariance of Brownian motion.
Its paths are continuous for . As , put . The given almost-sure limit gives
The Gaussian-process characterization of Brownian motion now proves the time inversion of Brownian motion:
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b

Words: 74 Articles: 1

Solution

Words: 74
Use the time-inverted Brownian motion . For , set . Then
As corresponds exactly to , and the inequality at is automatic because , this is the pathwise identity
Since and have the same law by time inversion of Brownian motion,
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c

Words: 142 Articles: 1

Solution

Words: 142
Let and . Split the crossing event according to its endpoint:
Under the Cameron-Martin theorem for a linear drift, the law of relative to standard Wiener measure has endpoint density
On paths that cross and end at , the Brownian reflection principle reflects the path after its first hit of and changes the endpoint to . Under this reflection the density becomes
The remaining exponential is the Cameron--Martin density for drift . Therefore
where the last equality uses the symmetry of the normal distribution. Subtracting the crossing probability from one gives
Equivalently, in terms of the standard normal distribution function,
This is the finite-horizon maximum of Brownian motion with negative drift formula.
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d

Words: 113 Articles: 1

Solution

Words: 113
By continuity of Brownian motion, the event that the last strict crossing of occurs by time is
Apply part (b) with and interchanged and its time parameter replaced by . This turns the right-hand side into
Part (c), now with drift , barrier , and horizon , gives
This is the distribution function of the last passage time above a level for Brownian motion with negative drift. Taking gives
the probability that the negatively drifted Brownian path never exceeds , consistent with the infinite-horizon crossing probability for Brownian motion with negative drift.
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30E (Asymptotic Methods)

Words: 276 Articles: 8

a

Words: 66 Articles: 1

Solution

Words: 66
The endpoints are the two classical turning points, determined by . Since the potential is even, they are symmetric. For , they lie in the linear part of the potential and satisfy ; for , they lie in the outer part and satisfy . Hence
The two-turning-point WKB quantization condition uses
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b

Words: 119 Articles: 1

Solution

Words: 119
By the evenness of , the semiclassical action integral is twice its integral over the positive half-axis. If , then
If , split the integral at :
The first integral is
In the second, put and then . It becomes
After simplification,
This is the action integral for a linear-to-square-root potential.
The graph begins at the origin, is continuous and strictly increasing, passes through , and tends to infinity. Therefore for every and , the equation
has exactly one solution by the intermediate value theorem and strict monotonicity.
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c

Words: 54 Articles: 1

Solution

Words: 54
For fixed , the right-hand side of the quantization equation tends to zero with . If
the unique energy satisfies , so the first branch of the action integral for a linear-to-square-root potential applies exactly. Solving
gives
Thus this formula is valid whenever
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d

Words: 37 Articles: 1

Solution

Words: 37
For , the outer part of the action integral for a linear-to-square-root potential dominates:
The WKB quantization condition therefore gives
Taking the power yields the asymptotic equivalence
Hence
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31A (Dynamical Systems)

Words: 448 Articles: 1

Solution

Words: 448
At an equilibrium, the second equation gives . The first equation then gives
Hence the fixed-point branches in the plane are
and
The three branches meet at . The branch meets the positive square-root branch again when , so the second bifurcation value is
The Jacobian matrix at a general point is
On the branch it is triangular, with eigenvalues
Thus is unstable for , asymptotically stable for , and unstable for .
On a square-root branch write . Then
whose trace is and determinant is . The negative branch is therefore a saddle equilibrium for every . The positive branch is a saddle for and asymptotically stable for ; close to it is a stable node.
To resolve the nonhyperbolic point at , make the prescribed substitution
and append . The equations become
The centre subspace is . Seek the extended centre manifold for a parameter as
The centre-manifold invariance equation is
To second order, , so comparison of coefficients gives
and hence , . Therefore
Substitution into the equation gives the reduced flow
Its central branch is unstable for and stable for , while the two nonzero branches for are unstable. Thus the bifurcation at zero is a subcritical pitchfork bifurcation with reversed normal-form parameter , exactly as recorded by the extended centre manifold of the 2023 Cambridge quadratic-product system.
The complete bifurcation diagram is therefore as follows. For , only exists and is unstable. For , is stable while both and are saddles. For , is stable while and are saddles. At , and cross and exchange stability, so the bifurcation is transcritical. This gives the bifurcation diagram of the 2023 Cambridge quadratic-product system.
Finally consider the phase plane near with . If , the lower equilibrium is a stable node and the upper equilibrium is a saddle. If , the lower equilibrium is the stable node and the upper equilibrium is the saddle. In each case the saddle has one-dimensional stable and unstable manifolds; one unstable separatrix runs toward the nearby stable node, while the other runs out of the local neighbourhood. The two equilibrium branches and their local invariant manifolds exchange roles as passes through one, which is the standard local phase portrait of a transcritical bifurcation.
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32E (Integrable Systems)

Words: 240 Articles: 4

a

Words: 124 Articles: 1

Solution

Words: 124
Let be the group parameter. The infinitesimal generator of a Lie point symmetry
has flow equations
Therefore it generates the scaling group
Here , , and . The total-derivative formulas for the second prolongation of a Lie point symmetry give
and
Thus
For the wave equation expression ,
It therefore vanishes whenever , proving that generates the simultaneous spacetime scaling symmetry of the wave equation.
The independent invariant of the scaling orbits is the similarity variable
while itself is invariant. Seek a group-invariant solution . Direct partial differentiation gives
The wave equation reduces to
Hence, on any interval avoiding ,
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b

Words: 116 Articles: 1

Solution

Words: 116
For
the flow equations are
with at . Solving the first two gives, with ,
Integrating the last equation then gives the one-parameter group
defined locally where .
To verify the symmetry infinitesimally, use
The needed coefficients of the second prolongation of a Lie point symmetry are
and
For the potential Burgers equation written as
we obtain
Thus the prolonged generator is tangent to the solution manifold , and the finite transformations above form the projective Lie symmetry of the potential Burgers equation.
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a

Words: 120 Articles: 1

Solution

Words: 120
For distinguishable particles with one-particle Hilbert spaces , the multiparticle quantum state belongs to
A product of one-particle states gives a product vector, and arbitrary linear combinations give entangled states. A noninteracting Hamiltonian is the sum of one-particle Hamiltonians acting on their respective tensor factors, so product-state energies add.
For two identical particles, the particle exchange operator swaps every degree of freedom. Since , its eigenvalues are . Particles whose allowed total states satisfy
are bosons, while those satisfying
are fermions. Thus bosonic states are symmetric and fermionic states antisymmetric under interchange. The same condition applies to every transposition in a system of more than two identical particles.
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b

Words: 156 Articles: 1

Solution

Words: 156
Spin-one particles are bosons, so their total two-particle state must be symmetric. Write for . A basis of symmetric spin states is
Denote these six states by . A basis of antisymmetric spin states is
This is the six-plus-three decomposition of two identical spin-one bosons.
In the ground orbital both particles occupy , so the spatial wavefunction
is symmetric. The complete list of ground states is therefore
At the first excited energy, one particle occupies and the other . The normalized symmetric and antisymmetric spatial states are
Overall bosonic symmetry permits symmetric spatial times symmetric spin and antisymmetric spatial times antisymmetric spin. Hence all first excited states are
The ground and first excited degeneracies are therefore six and nine.
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c

Words: 133 Articles: 1

Solution

Words: 133
Write the equally spaced one-particle spectrum as
The two-particle level labelled by has energy
and receives contributions from orbital pairs with .
For every unequal unordered pair , there is one symmetric and one antisymmetric spatial combination. The symmetric one combines with the six-dimensional symmetric spin space; the antisymmetric one combines with the three-dimensional antisymmetric spin space. Thus each unequal pair contributes nine states.
If is odd, all pairs are unequal and there are unordered pairs. Therefore
If is even, there are unequal pairs and the additional equal pair . The latter has only a symmetric spatial state and therefore contributes six spin states. Hence
This is the degeneracy of two identical spin-one bosons with equally spaced orbital levels.
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Solution

Words: 238
Let the Bravais lattice have primitive vectors , and put
The reciprocal lattice has the basis
The scalar triple product and cross product identities give
Consequently every satisfies for every lattice point , and conversely these three conditions force the coefficients of in the reciprocal basis to be integers. This proves that the displayed vectors generate .
In the Born approximation, suppose that the crystal potential is the sum of translates of one atomic potential over the finite set of lattice sites. Its Fourier transform at the momentum transfer factors as
Thus the single-atom scattering amplitude is multiplied by the crystal lattice structure factor . Writing
separates the sum into three finite geometric series. For this gives
When the are large, a factor has a sharp maximum when . All three factors are therefore simultaneously large precisely when . These are the reciprocal-lattice peaks of a finite crystal.
For the stated Body-centered cubic lattice basis,
the reciprocal-basis formula gives
Equivalently,
The shortest nonzero reciprocal vectors have squared Euclidean norm , so
In elastic scattering, . If and is the angle between and , Euclidean geometry gives
The first possible diffraction peak therefore occurs at
as , by the small-angle approximation. This is the elastic Bragg scattering condition for the shortest reciprocal-lattice vector.
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35A (Statistical Physics)

Words: 281 Articles: 11

a

Words: 54 Articles: 1

Solution

Words: 54
For an ideal gas of identical bosons, the Bose-Einstein distribution gives the mean occupation of a discrete one-particle state as
where is the chemical potential. If the spectrum is sufficiently dense to use a density of states , the discrete sum becomes
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b

Words: 227 Articles: 8

i

Words: 65 Articles: 1
Solution
Words: 65
Use periodic boundary conditions on the square crystal. Each allowed wavevector occupies area in two-dimensional -space. Including the two phonon polarizations, the number of modes in the disk is
The phonon dispersion relation gives , so
Differentiating the cumulative mode count produces the density of states for a two-dimensional power-law phonon dispersion:
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ii

Words: 32 Articles: 1
Solution
Words: 32
The Debye model fixes its cutoff by requiring the continuum to contain the vibrational degrees of freedom:
Therefore the Debye frequency and Debye temperature are
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iii

Words: 37 Articles: 1
Solution
Words: 37
A phonon has zero chemical potential and energy . The total internal energy is consequently
With the change of variable and , this becomes
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iv

Words: 93 Articles: 1
Solution
Words: 93
For , the preceding density of states has
When , the Bose-Einstein distribution has the classical approximation
Each of the modes therefore contributes to the energy, so the Dulong-Petit law gives
When , the upper integration limit tends to infinity. The Bose integral
then yields
Hence the heat capacity at constant volume is
so . The high-temperature constant is the classical equipartition theorem result, while the low-temperature power law makes as required by the Third law of thermodynamics.
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36A (Electrodynamics)

Words: 289 Articles: 8

a

Words: 71 Articles: 1

Solution

Words: 71
The electromagnetic four-potential is the field generated by the four-current : every source volume element contributes with the inverse-distance Green-function factor. Electromagnetic influence propagates at speed , so causality requires the source to be evaluated where its worldline intersects the field event's past light cone. Thus
The source time is exactly the retarded time , rather than the observation time .
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b

Words: 45 Articles: 1

Solution

Words: 45
Put
Because , differentiation gives
A massive charge has the subluminal speed , so . Hence is strictly increasing, and has at most one root. This is the uniqueness of retarded time for a subluminal source.
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c

Words: 88 Articles: 1

Solution

Words: 88
For a point charge, the charge density and current density are
Insert these into the retarded electromagnetic potential. The argument of the Dirac delta function depends on through
At its unique zero , the Jacobian determinant contributes the factor
Since the source is subluminal, this quantity is positive. Writing , , and evaluating at gives the Lienard-Wiechert potentials
The identity equivalently gives .
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d

Words: 85 Articles: 1

Solution

Words: 85
Assume that is constant. Set
Implicit differentiation of gives
Since , direct differentiation of yields
Therefore
The Lienard-Wiechert potentials for uniform motion have and . The preceding identity consequently implies
As is constant,
Thus the explicit uniformly moving potentials satisfy the Lorenz gauge.
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37B (General Relativity)

Words: 393 Articles: 13

a

Words: 296 Articles: 10

i

Words: 62 Articles: 1
Solution
Words: 62
The radial first integral for an equatorial null geodesic in Schwarzschild spacetime is
Since , regarding as a function of gives
Set . Then and therefore . Division by gives the equatorial null orbit in Schwarzschild spacetime
where is the impact parameter. Differentiating with respect to gives
By continuity this yields
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ii

Words: 62 Articles: 1
Solution
Words: 62
In the flat-spacetime limit , the orbit equation is the harmonic oscillator equation
Its general solution is . The conditions , hence , at and set . Choosing at closest approach fixes , so
This is a straight line at perpendicular distance from the origin in polar coordinates.
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iii

Words: 50 Articles: 1
Solution
Words: 50
Write
where is first order in . Substitution into and omission of terms of order and gives
This is the linearized orbit equation used in the perturbative derivation of Schwarzschild light deflection.
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iv

Words: 56 Articles: 1
Solution
Words: 56
The homogeneous solution is
For the constant and forcing terms, a particular solution is
Indeed, applying multiplies the coefficient by . Thus
The term only changes the definition of at this order, so one may set .
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v

Words: 66 Articles: 1
Solution
Words: 66
Demanding that the incoming ray comes from infinity at means . The solution from part (iv) then gives
At the outgoing end write , where is first order in . Then
whereas
The condition therefore gives
Restoring units gives , the leading Schwarzschild light deflection.
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b

Words: 97 Articles: 1

Solution

Words: 97
An affinely parameterized geodesic satisfies
For the conformally flat metric , its Christoffel symbols are
Let . Along a null geodesic, , so the equation reduces to
The acceleration is parallel to the tangent. A change of parameter removes it, leaving a straight null line of the Minkowski metric. Thus conformal rescaling changes the affine parameter but not the unparametrized light ray.
Consequently Nordstrom theory of gravitation predicts
for light passing a star. This contradicts the observed nonzero deflection and the successful general-relativistic value .
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38C (Fluid Dynamics II)

Words: 361 Articles: 10

a

Words: 79 Articles: 1

Solution

Words: 79
Let be a representative positive gap thickness and set
the larger-order horizontal speed after including the squeeze-induced flux. The lubrication-limit scaling for a moving thin gap requires
Equivalently, the inertial condition contains
The gap must also remain open, . These conditions make streamwise derivatives small relative to transverse derivatives, keep the pressure uniform across the gap to leading order, and reduce the Navier-Stokes equation to Stokes flow locally.
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b

Words: 41 Articles: 1

Solution

Words: 41
The leading streamwise momentum equation in lubrication theory is
with . The no-slip boundary condition is
Twice integrating in gives the local Couette-Poiseuille flow in a thin gap
Its volume flux per unit span is
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c

Words: 84 Articles: 1

Solution

Words: 84
Integrating the incompressible continuity equation across the moving gap, with and , gives the Reynolds lubrication equation
Hence
for a constant , and the flux formula from part (b) gives
Define the spatial mean
Because both ends meet fluid at pressure , the pressure recovery condition in lubrication flow is
It determines
Therefore the requested pressure gradient in a translating and squeezing finite gap is
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d

Words: 64 Articles: 1

Solution

Words: 64
When , put
The pressure gradient from part (c) reduces to
Because , is a weighted mean of points in and therefore belongs to ; it lies strictly inside unless the weight is singularly concentrated at an endpoint. Thus , proving that the pressure gradient vanishes somewhere between the ends.
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e

Words: 93 Articles: 1

Solution

Words: 93
The leading shear stress exerted by the fluid on the lower surface is
The horizontal force per unit span is . Substituting the pressure gradient from part (c) gives
Using the value of and setting this force to zero yields
Consequently the zero-shear lower wall in a translating and squeezing finite gap condition is
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39C (Waves)

Words: 350 Articles: 14

a

Words: 120 Articles: 6

i

Words: 28 Articles: 1
Solution
Words: 28
Substitute the monochromatic wave
into the differential equation. Since , cancellation of the common exponential gives
Thus the dispersion relation is
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ii

Words: 57 Articles: 1
Solution
Words: 57
From the dispersion relation, the phase velocity and group velocity are
Both are even functions of , both attain their minimum value at , and both increase like . For every ,
The graph of therefore lies above the graph of away from their common minimum.
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iii

Words: 35 Articles: 1
Solution
Words: 35
A wave crest moves at the phase velocity, while the envelope of a narrow wave packet moves at the group velocity. Since for every nonzero wavenumber, the crests move more slowly than the packet.
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b

Words: 230 Articles: 6

i

Words: 90 Articles: 1
Solution
Words: 90
The Fourier modes evolve according to the dispersion relation found in part (a), so
For , the stationary-point equation is
It has the two real solutions
Define
The one-dimensional stationary-phase formula gives one contribution from each stationary point:
Because the initial field is real, its Fourier transform has the conjugate symmetry . Hence the same result can be written
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ii

Words: 57 Articles: 1
Solution
Words: 57
If the initial field is also an even function, then is real and even. Provided , the leading term becomes
Its large zeros satisfy
Therefore
If , the leading stationary-phase coefficient vanishes and a higher-order term determines the zeros.
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iii

Words: 83 Articles: 1
Solution
Words: 83
For ,
for every real , so there is no real stationary point. The ray travels more slowly than the minimum group velocity and receives no leading stationary-phase wave packet. Under the usual smoothness and decay assumptions on , the nonstationary oscillatory integral can be integrated by parts repeatedly, so
for every fixed for which the needed derivatives are integrable. In particular it is asymptotically much smaller than the signal when .
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40C (Numerical Analysis)

Words: 356 Articles: 8

a

Words: 107 Articles: 1

Solution

Words: 107
For
the gradient is . The steepest descent method with exact line search for a positive-definite quadratic therefore uses
For and , the minimizer is . Put
Starting from , direct substitution gives and, inductively,
The Euclidean norm is unchanged by the alternating sign, so
For a positive-definite matrix, the spectral condition number of a positive-definite matrix is
Here , and hence
The Conjugate gradient method starts with and updates
By finite termination of the conjugate gradient method, it reaches the exact solution in at most the number of distinct eigenvalues. This matrix has two, so at most
are required in exact arithmetic.
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b

Words: 89 Articles: 1

Solution

Words: 89
Since , the Heavy-ball method is
Multiplication by and use of give the heavy-ball residual recurrence
With the usual initialization , both initial residuals equal . Induction in the recurrence shows that
for a polynomial of degree at most . Therefore
This is under the zero-indexed Krylov subspace convention in the question; under the convention whose order- space ends at , it is .
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c

Words: 55 Articles: 1

Solution

Words: 55
Because , the error obeys
Thus the heavy-ball error propagation matrix is
If , permute the coordinates from
to
For the corresponding permutation matrix ,
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d

Words: 105 Articles: 1

Solution

Words: 105
Put . Then
For an eigenvalue , the corresponding block has characteristic polynomial
For ,
so the polynomial is
For , it is
Its discriminant is , so its conjugate roots have product and modulus . Both blocks therefore have the same spectral radius, and
This is the heavy-ball rate for a two-eigenvalue diagonal quadratic.
By contrast, the steepest-descent factor is
The heavy-ball factor is , which is substantially smaller for : it gives an iteration scale of order rather than order .
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