Starting with , definewhile the denominator is nonzero. This gives the simple continued fractionA finite expansion is rational by evaluating it from the bottom. Conversely, for rational , these steps are the Euclidean algorithm applied to numerator and denominator, so the remainders eventually vanish.
Define convergents byThe recurrence givesso induction yieldsIn particular,Since an irrational lies strictly between these convergents, the two approximation errors sum to this distance. If both displayed bounds in the question failed, their sum would be at leastby the arithmetic-geometric mean inequality, contradicting strict betweenness. Thus at least one bound holds.
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Runge approximation theorem in its polynomial form says that if is compact with connected complement and is holomorphic on a neighborhood of , then polynomials approximate uniformly on .
The assertion is true when “uniform” means on all of the unbounded quadrant . A uniformly convergent sequence is uniformly Cauchy. For sufficiently large , the polynomial is bounded on . Every nonconstant polynomial is unbounded along some ray contained in , so is constant. Fixing one large , the limit is therefore plus the limit of constants, hence is a polynomial.
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The assertion is true. Exhaust the quadrant by compact sets with connected complements and with every compact subset of eventually contained in the interior of . Runge's theorem gives a polynomial satisfyingThus locally uniformly. For a fixed , choose a small circle about eventually contained in every . The Cauchy integral formula for derivatives applied to givesfor every .
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Let be the matrix whose columns are the distinct nonzero vectors of . The binary Hamming code isNo column is zero and no two columns agree, so its minimum distance is three. A radius-one Hamming ball containswords, while . The radius-one balls about codewords are disjoint and their total size is , so they partition the ambient space. Hence is a perfect code.
Let the received word be all ones except in the last coordinate. The sum of all nonzero vectors of is zero for , so its syndrome is the last column of . Minimum-distance decoding therefore flips the last bit and returns the all-one word. A Hamming code corrects every single error because each nonzero syndrome identifies its unique erroneous coordinate.
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A regular expression is built from , , and alphabet symbols using union, concatenation, and Kleene star; its language is defined by applying the corresponding set operations recursively. A deterministic finite automaton is a tuple and acceptsKleene theorem says that the languages denoted by regular expressions are exactly those accepted by finite automata.
Regular languages are closed under finite union, using a product automaton or nondeterministic choice, and under finite intersection, using the product automaton with accepting set .
They are not closed under countable unions or intersections. Every language over a finite alphabet is a countable union of singleton languages, each regular, so a nonregular language such as is a counterexample. It is alsoa countable intersection of regular languages, giving the second counterexample.
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Assume has full column rank. The log-likelihood, up to constants, isThe ordinary least squares normal equations giveand maximizing over the variance gives the maximum-likelihood estimatorBecause is an orthogonal projection of rank ,Writing for the -quantile, a confidence interval of level is
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The boundary condition says that all newborn individuals enter at age zero, and that their influx equals the total birth rate obtained by summing the age-specific births over the population.
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Substitution into the renewal boundary condition and cancellation of gives the Euler-Lotka equationThis is the necessary condition selecting the growth exponent .
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For and constant death rate ,ThusA separable solution exists with this exponent, and it grows precisely when
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For any , choose with and defineThe recurrence makes this independent of and agrees with the original integral where . It is the desired analytic continuation away from the listed points.
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Usingwe see that is generally a simple pole, inherited from . A cancellation occurs exactly when is a nonpositive integer. Thus is always a simple pole; for , is removable when is one of , and otherwise is a simple pole.
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The scalar and vector potentials satisfyThe canonical momentum and Hamiltonian areFor the uniform fields choosewhich produces the stated Hamiltonian. Since it is time independent and are cyclic coordinates, three independent conserved quantities are
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InsertMatching powers of requires , so . Writing , the scalar equation and Friedmann equation giveThusExistence with positive potential requires , or . Accelerated expansion requires , hence
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The acceleration equation requires , so . A canonical scalar field with nonnegative potential obeys . Hence inflation occurs for
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Without Alice's operation, Bob obtains outcome with probabilityIf Alice applies and then measures, but her outcome is not communicated, Bob's probability isbecause . Equivalently, a trace-preserving local operation leaves Bob's reduced density matrix unchanged. This is the no-communication theorem: local operations cannot signal without communication of their outcomes.
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Two integral binary quadratic forms are properly equivalent when one is obtained from the other by a change of variables in . For a negative discriminant , the class number of binary quadratic forms is the number of proper equivalence classes of primitive positive-definite forms of discriminant .
If properly represents , then for coprime . Extend to a matrix in ; after the associated variable change, the coefficient of is , so the transformed form isThe converse follows by evaluating this form at .
Such a form has discriminant precisely whenso it exists exactly when . Thus is properly represented by some form of discriminant exactly when is a square modulo .
Now let . If is composite for , it has a prime divisor , andConversely, if is a square modulo for a prime , choose an odd square root with . Then and , so that value is composite.
Finally, reduction theory says that every nonprincipal positive-definite class of discriminant has a reduced representative whose leading coefficient has a prime divisor for which is a square modulo . Conversely such a prime produces a represented form not equivalent to the principal form . Combining this with the preceding equivalence gives
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A parse tree has the start variable at its root; the ordered children of a variable spell the right side of the production used at that occurrence, and its leaves, read left to right, spell the derived word.
For a grammar in Chomsky normal form with variables, take pumping length . A parse tree for a word of length at least has a root-to-leaf path containing one variable twice. The yield can therefore be writtenwhere , , and replacing the subtree between the repeated variables zero, one, or several times provesThis is the pumping lemma for context-free languages. Without Chomsky normal form but with no epsilon or unit productions, use the maximum production length to choose a larger exponential ; bounded branching and the same repeated-variable argument apply.
The language is not context free. A pumped window of bounded length cannot alter all three long blocks equally, so pumping breaks one of the required equalities.
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The language is context free. For example the grammargenerates with , and every required word has this form.
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The language is not context free. Intersecting with a suitable regular language that forces both copies into long homogeneous blocks reduces to a marked copy language; the context-free pumping lemma then places the two pumped pieces within only finitely many local blocks and cannot change the two copies identically. Equivalently, the standard copy-language proof applies with the fixed marker .
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The term moves susceptible people in group into its infective class, while moves infectives into recovery. In is the contact rate of a person in group with group , and is the infectious fraction there. The reciprocity condition says that the total number of -- contacts agrees when counted from either group. Common and mean age-independent transmission per infectious contact and recovery rate. There is no transmission between distinct age groups exactly when
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With , the infective equations becomewhere reciprocity was used. For a column vector ,Therefore
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Since and have the same eigenvalues, an exponentially growing mode exists precisely when has an eigenvalue with real part greater than one. For the nonnegative contact matrix this iswhere is the spectral radius.
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Substituting into the continuity equation givessoThree powers arise from dilution of photon number in physical volume and one from the cosmological redshift of each photon's energy.
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The positive-curvature term identifies as the curvature radius of the spatial three-sphere when the dimensionless scale factor is ; the physical curvature radius is .
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Put withThenFor this becomesThe expanding big-bang branch hasDifferentiation givesThus, with ,where the initial derivative givesFor , expands forever and becomes asymptotically exponential. For , it reaches a maximum and recollapses to zero. At , increases monotonically to , the limiting static radius.
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Writewhere is the normalized component orthogonal to . On this real plane, is reflection in the line perpendicular to , whileis reflection in the line spanned by . Their product is a rotation through toward . This is the geometric core of Grover search.
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Prepare . One query to , with phase kickback, implements . The reflection is independent of and can be implemented by conjugating the phase flip of with . Since begins at angle from the unmarked direction, one Grover iterate rotates it by and givesA computational-basis measurement therefore determines with certainty after one oracle query.
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Let and . Since , choose with , . Normalizing the two nonzero projections givesAt an endpoint, the unused normalized vector may be chosen arbitrarily in its subspace.
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The two stated formulas show that rotates the plane by . Starting from , whose angle from is , two iterations give angleHence . The reflection about is implementable asThus apply to , followed by two applications of . This prepares exactly and deterministically.
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For cardinals, means that there is an injection but no bijection. Under the axiom of choice, every set is well-orderable, so every infinite cardinal is the initial ordinal for a unique ordinal . Cantor theorem givesand minimality of the successor cardinal givesThe strict inequality printed in the conversion is not provable and can be false under the generalized continuum hypothesis; the intended symbol must be .
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The map injects into . Cantor's diagonal argument shows that no map is surjective: for , the set differs from every . Hence .
If is surjective, inverse image gives an injectionFor every infinite initial ordinal , transfinite recursion constructs a pairing of with : at each stage fewer than earlier pairs have been used. Thuswithout invoking choice for arbitrary families.
Every ordinal below has cardinal at most and can be coded by a well-ordering relation on a subset of . Sending such a relation to its order type, and all non-well-orders to zero, gives a surjectionUsing the pairing above to code relations as subsets of yieldsAgain, strictness beyond this is independent of the usual axioms.
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The diagonal Ramsey number is the least such that every red-blue coloring of contains a monochromatic . The standard recursiongivesThus the converted is a superscript-order error; that bound is false for large .
In a red-blue coloring, if the red spanning graph is connected it has a red spanning tree. Otherwise its red components are joined pairwise by blue edges, making the blue graph connected, so it has a blue spanning tree.
The result fails for three colors. Color the six edges of by its three perfect matchings, one color per matching. Every monochromatic graph then consists of two disjoint edges and has no spanning tree.
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A directed path of length two is determined by its middle vertex and an ordered pair of distinct neighbors, givingFor the colored complete graph, letA monochromatic triangle contributes three monochromatic two-edge angles to , while a nonmonochromatic triangle contributes one. If and are their respective numbers, thenEliminating gives
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The elementary symmetric functions areThe Fundamental theorem of symmetric polynomials says that every symmetric polynomial is uniquely a polynomial in .
If are the roots of a monic polynomial, its discriminant isThis is symmetric in the roots, hence the theorem and Vieta's formulas express it polynomially in the coefficients. Equivalently,For this givesFor , a repeated root solves . Elimination givesThus the discriminant vanishes exactly when or .
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For an -module ,The action is left multiplication on the first factor:It is well defined because the tensor relation is preserved by left multiplication.
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If the -classes in have representatives , the induced-character formula isIt follows by grouping the standard sum over satisfying .
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The subgroup is the unique Sylow-seven subgroup and is normal. No element outside it centralizes , so . Similarly has order three. Thus nonidentity powers of form two classes of size three, while the elements of orders three form two classes of size seven. Together with the identity, there are five conjugacy classes.
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Let and let . Conjugation by partitions the six nontrivial characters of into the two orbitsInducing one representative from each orbit gives two irreducible degree-three characters . On the five classes represented by their values arewith the two cyclotomic sums interchanged for . Their squared degrees, together with the three linear characters, sum toso these are all irreducible characters.
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Triangulate and adjoin one new vertex joined to every simplex; the resulting simplicial complex realizes the cone . The cone contracts to its apex, so
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Write . After replacing the two pieces by small open neighborhoods, their intersection deformation retracts to . The Mayer-Vietoris sequence, together with for and , becomesand at degree zero ends aswhich is the required sequence.
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Attaching the cone collapses the circle in the torus. The quotient has the homotopy typeEquivalently, the exact sequence in part (b) kills one of the two generators of and preserves the fundamental two-cycle. Therefore
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A family of continuous functions on a compact space is equicontinuous if, for every and every , there is a neighbourhood of such that for every in and every in . The Arzela-Ascoli theorem says that has compact closure in with the uniform norm if and only if it is equicontinuous and pointwise bounded.
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Apply Arzela-Ascoli theorem on . Pointwise boundedness and equicontinuity give a subsequence converging uniformly there. Successively extract subsequences for , and take the diagonal subsequence. It converges uniformly on every closed bounded interval. Its limits on nested intervals agree, so they define on the real numbers; the locally uniform limit of continuous functions is continuous.
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Fix and . Since is compact in the uniform norm, choose a finite -net . By continuity, there is a neighbourhood of on which for every . For in , choose with . The triangle inequality gives on , uniformly in . Thus is equicontinuous.
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A locally compact Hausdorff space is regular. Cover by finitely many open sets whose compact closures lie in ; their union satisfies , with compact. The compact Hausdorff space is normal, so the Urysohn lemma gives a continuous function equal to on and on . Extend by zero outside . The boundary values make the extension continuous, and its support is a compact subset of .
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The Riemann-Lebesgue lemma states that the Fourier transform of an function is continuous and tends to zero at infinity.
For a Schwartz function , differentiation under the integral and integration by parts giveThe Riemann-Lebesgue lemma bounds the right side by an seminorm of . Every Schwartz seminorm of is therefore bounded by finitely many Schwartz seminorms of . Hence the Fourier transform maps continuously into itself.
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Taking the Fourier transform of a derivative givesThus, away from ,This formula determines the solution uniquely; a distribution supported only at cannot belong to unless it is zero.
For , the Fourier transform estimate and local integrability of in three dimensions control the squared norm. For ,The Plancherel theorem therefore yields . Finally the Sobolev embedding theorem in three dimensions gives when , namely when .
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A point is ramified with multiplicity exactly when it is a zero of of multiplicity . Since has degree , the fundamental theorem of algebra gives .
Conversely, choose distinct complex numbers and put with . The assumption makes a polynomial of degree . Any antiderivative of has degree and precisely the prescribed ramification multiplicities.
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Outside the finite set of branch points, the derivative is nonzero. The inverse function theorem supplies evenly covered neighbourhoods, and compactness of the Riemann sphere makes every fibre finite, so the restriction is a covering map.
Lift a loop from each point of the fibre over ; its endpoints define a permutation . The homotopy lifting property shows that this permutation depends only on the based homotopy class. The punctured source is connected, so a path between any two points in the fibre projects to a loop whose lift joins them. Hence the monodromy group acts transitively.
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The monodromy around both and must be a product of two disjoint transpositions, hence a cycle type in . The product relation for loops around the three punctures says . By the stated fact, is either the identity or another permutation. Consequently cannot contain a -cycle. But ramification index over infinity would force exactly such a cycle, a contradiction.
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A projective variety is smooth when every local ring is regular, equivalently when its Jacobian has the expected rank at every point. The affine curve is smooth because the derivative of with respect to is , while its projective closure is singular at .
The genus is . Intersect the Fermat cubic threefold with the plane . This gives the smooth plane cubic , whose genus of a smooth plane curve is .
An irreducible plane conic is smooth: a singular quadratic form in three variables has rank at most two and factors over the algebraically closed field, contradicting irreducibility. Projection from any point of the conic, or its degree-two complete linear system, then identifies it with the projective line.
Finally, a nonzero ternary quadratic form is determined up to nonzero scalar by its six coefficients. Thus generalized conics are parametrized bijectively by .
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Write a conic as for a symmetric matrix , with off-diagonal entries equal to half the corresponding coefficients. A union of two distinct lines has matrix rank two. Thus is the rank-two part of the determinant hypersurface . Its closure also contains rank-one matrices, representing double lines, so it is not Zariski closed. Since the determinant is one nonzero homogeneous equation in , its dense rank-two locus has dimension .
The final sentence of the converted question writes , but the natural intended set is . The homogeneous ideal of its closure is the principal ideal generated by the cubic polynomial : the determinant hypersurface is irreducible, and is dense in it.
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A point is a regular value of when every derivative for in is surjective. Sard theorem says that the critical values of a smooth map have measure zero. The stack-of-records theorem says that the inverse image of a regular value is a smooth submanifold of codimension .
Maps and are smoothly homotopic when a smooth has endpoint maps and . Perturb such a homotopy relative to its ends so that it is transverse to . Then is a compact one-dimensional manifold whose boundary is . Every compact one-dimensional manifold has an even number of boundary points, proving the parity formula.
The hypothesis on says that the degree modulo two of is one. Suppose no and were antipodal. Thenwould be defined, even, and homotopic to by normalized straight-line interpolation. For a regular value, the fibres of the even map occur in antipodal pairs, so its degree modulo two is zero. Homotopy invariance gives a contradiction. Hence some antipodal pair is mapped to an antipodal pair.
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If the variables are independent random variables, apply the defining product rule first to indicator functions, then to simple functions, and finally use bounded measurable approximation to obtain the displayed identity. Conversely, choosing giveswhich is independence.
Let . Independence and zero means imply orthogonality in , soIf the variance series converges, is Cauchy in the complete space and hence converges there. Conversely, convergence makes Cauchy, so every tail of the nonnegative variance series tends to zero; therefore .
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The queue length is a birth-death process with birth rate in state and death rate . Its reversible weights satisfyFor , the factor makes their sum finite for every . For , the tail is geometric with ratio , so a stationary distribution exists exactly when .
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On states , births have rate below and deaths have rate above . For this finite continuous-time Markov chain is irreducible, so its unique stationary law isFor this is uniform. If the parameter value is admitted, state is absorbing and the unique stationary law is instead the point mass at .
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In equilibrium the chain is reversible by detailed balance. Reverse time. Forward departures become reverse accepted arrivals; reversibility identifies the reversed chain with the original one, whose attempted arrivals form a Poisson process. The accepted points are exactly those occurring while the state is below . The standard quasi-reversibility argument therefore makes the equilibrium departure process Poisson, with rate equal to the mean departure rate
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The log-likelihood is, up to constants, , so the maximum-likelihood estimator is . By the central limit theorem,Applying the delta method to gives
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Let be the corresponding standard normal distribution quantile. Slutsky theorem permits replacing by the consistent estimator , giving the confidence intervalAfter standardization, the preceding convergence in distribution and continuity of the normal distribution show that its coverage tends to .
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For bootstrapping, repeatedly sample with replacement from the empirical distribution of the observations and compute . Conditional on the data, estimate the and quantiles of . The basic bootstrap interval isAs the number of resamples tends to infinity it estimates the conditional quantiles; bootstrap consistency and the continuous mapping theorem then give asymptotic coverage .
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For a bounded stopping time , writeThe indicator is measurable at time . Taking conditional expectations term by term and using the supermartingale inequality gives . The same calculation gives equality for the martingale . Since their initial values agree, .
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If shares are held during period , the remaining wealth is in the bank account. Self-financing therefore giveswhich rearranges to the required equation.
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Condition on the information through time . Independence of and the definition of the Bellman equation for terminal-wealth utility implybecause the actual holding is one candidate in the supremum. Thus is a supermartingale for every strategy.
For the stated strategy it is a martingale, soEvery competing strategy has expected terminal value at most by the supermartingale inequality from part (a), evaluated at the bounded time . Hence is optimal.
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One form of Watson lemma is this. If has the asymptotic expansion as , with , and the Laplace integral has suitable growth control away from zero, thenas , with truncation after any fixed number of terms justified by the corresponding remainder estimate.
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Complete the square: . The pole of is at , so the contour may be shifted upward through the saddle point without crossing a singularity. Setting gives the exact steepest-descent representationNear the saddle,Odd terms integrate to zero, whileThe Watson lemma therefore yields the full asymptotic expansion
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The second equation gives . The first then says either , giving the persistent equilibrium points and , orgiving and . These two points exist for .
At the origin the Jacobian matrix has trace and determinant , so it is stable for and a saddle point for . At the trace is and determinant , so it is stable for and a saddle for . Stationary bifurcations occur atwith the first two coinciding when .
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At a non-axis fixed point the determinant and trace areThese formulas determine the solid stable and dashed unstable branches in the bifurcation diagram. The pair is born in a saddle-node bifurcation at . For , it exchanges branches with at and with at , both transcritical bifurcations. If , the saddle-node lies to the left of ; if , it lies to the right. For , the saddle-node and the collision at combine into a pitchfork bifurcation at .
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Put , , and , adjoining . ThenThe zero eigenvalue has centre direction . Solving the center manifold invariance equation givesSubstitution yields the reduced equationIts equilibria are and for , exactly matching the three branches meeting at the pitchfork in part (b).
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For small, has two negative eigenvalues and is a stable node. The two nearby equilibria satisfy and are saddles. Their stable and unstable separatrices form the local phase portrait; trajectories in the wedge between the stable manifolds approach , while trajectories crossing an unstable direction leave the neighbourhood.
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The transformations obey and is the identity. If , then . Thus solutions of the free-particle equation are mapped to solutions, so this is a one-parameter group of Lie symmetries.
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The flow equations of the displayed vector field are and . Hence , whose solution is . The vector field therefore generates the stated phase rotation.
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Direct substitution gives . Differentiating at gives .
Writing the transformed field in transformed coordinates givesConsequentlywhere . These formulas, together with their complex conjugates and the analogous mixed derivatives, give the second prolongation. Differentiating at zero yields
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Substituting the prolonged formulas showsso the nonlinear Schrödinger equation is invariant. Applying the symmetry to the given solitary wave produceswhich travels with speed .
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The addition of angular momentum rule givesFor each such , measurement along any axis has magnetic quantum number .
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For two equal spins, exchange acts on the coupled state by the Clebsch-Gordan coefficient symmetry factor . It is therefore when , making every state in that multiplet antisymmetric, and when , making the next multiplet symmetric.
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Parity conservation and the negative parity of require odd orbital angular momentum . Since the two particles are identical bosons, their spin state must then be antisymmetric, so their total spin is . Total angular momentum zero forces .
Conditioning on spin projection leaves orbital projection . The angular density is therefore proportional to . Including the solid-angle measure, the requested probability is
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A Bravais lattice is the integer span of three linearly independent primitive vectors. Its reciprocal lattice consists of vectors satisfying for every lattice vector .
Translations by lattice vectors commute with the Hamiltonian. Their simultaneous eigenvalues have the form , so an energy eigenfunction may be chosen withThus with lattice-periodic , which is Bloch theorem. Wavevectors differing by a reciprocal-lattice vector describe the same translation character, and the Brillouin zone is a fundamental Wigner-Seitz cell of the reciprocal lattice.
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TakeTheir integer span consists exactly of the cubic points together with the body-centre points, so the BCC set is a Bravais lattice. Using the inverse matrix supplied in the question, reciprocal primitive vectors areThese generate a face-centred cubic lattice; thus the reciprocal lattice of BCC is FCC, with the displayed scale.
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One quantum state occupies volume in wavevector space. Counting the shell of radius and including spin degeneracy givesUsing gives the stated power with
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The Bose-Einstein distribution isPositivity requires not to exceed the ground-state energy, here zero. For a finite system above the condensation limit one has ; it approaches zero from below at Bose-Einstein condensation.
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In the continuum limit the number outside the ground state isAt the largest allowed chemical potential, , the integrand behaves near zero as . The integral is finite exactly when . Excess particles must then occupy the ground state, so a Bose-Einstein condensate exists precisely for .
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For a point charge, , so the radiation fields are transverse and satisfy . The radial Poynting vector isChoosing the acceleration as polar axis and integrating over the sphere gives . Hence the Larmor formula is
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Ignoring the small radiative back-reaction, conservation of energy gives and Newton's equation gives . Integrating the Larmor formula with yields, for ,If , the particle turns at defined by and traverses the accelerated region twice, so the same formula holds with twice the integral from to .
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For , direct integration givesandThe reflected expression increases up to threshold and the transmitted expression decreases above it. The supremum is therefore approached from below at and equals
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The upper-left block has eigenvalues and , while the remaining two eigenvalues are both . The metric signature is therefore up to sign convention. It is Lorentzian.
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Let , define the tortoise coordinate by , and set the advanced time . Since , substitution givesThese are Ingoing Eddington-Finkelstein coordinates; all coefficients are regular at the event horizon .
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Outside the ingoing null shell the enclosed mass is , so use the ingoing Ingoing Eddington-Finkelstein coordinatesThis is the Schwarzschild metric of mass , regular across and valid for on the exterior side of the shell.
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Inside the spherical shell the enclosed mass vanishes by the spherical vacuum solution, so spacetime is flat. In the same ingoing coordinates,valid for on the interior side before the shell reaches the centre.
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Because the shell lies well inside its Schwarzschild radius once it reaches , an event horizon forms and the final exterior is a black hole of mass . In the ideal instantaneous-shell model the collapse ends at a spacetime singularity.
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The sink speed scales as , so the Reynolds number is . The approximation applies in the high-Reynolds-number region . Radial inertia scales as , so the radial pressure gradient has the same dependence.
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The definitions through the Stokes stream function giveso incompressibility is automatic.
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The similarity form givesUsing the outer pressure gradient in the correctly written radial boundary-layer equation givesNo slip and matching to the sink require and . The boundary-layer flux is of order , relative to the sink flux it isMass conservation therefore requires an outer correction of this relative size, which is small in the assumed region.
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Substitution of the monochromatic ansatz givesThus the outer solutions oscillate with and the middle solutions are combinations of and . The incident wave has phase ; its group velocity is upward, whereas the reflected sign has downward group velocity. The transmitted wave must again use the upward-energy sign. This gives exactly the three forms stated.
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Continuity of normal velocity and pressure at each density interface requires continuity of and at . These four conditions determine the four unknown amplitudes.
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Matching at first expresses the middle solution in terms of . Propagating its value and derivative across the layer of thickness uses the transfer matrixMatching this result to and at , then eliminating , gives
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Taking the squared modulus and using givesThe incident wavevector makes an angle with the downward vertical, so . Substitution gives the required formula.
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For the discrete Fourier mode , the centred second difference has multiplier . Hence the amplification factor isFor every , . The discrete Parseval identity then shows directly that the discrete norm cannot increase at any time step, proving unconditional stability for the Cauchy problem.
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Let be the symmetric Dirichlet second-difference matrix. Its eigenvalues are nonpositive, so every eigenvalue ofhas modulus at most one. Thus .
Insert the exact smooth solution into the scheme. The local truncation error per step has discrete norm , from the order-three trapezoidal time residual and the order-two centred spatial residual. If is the grid error, stability and iteration giveThere are at most steps and , henceThis proves convergence for every without invoking the Lax equivalence theorem.
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