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An integral positive definite binary quadratic form
is reduced when
with when or . Its discriminant is .
For , reduction gives , so or . Since , is even. If , then forces , and . If , then ; integrality of
leaves and , and the boundary convention retains only . Hence the complete list is
Now suppose the prime is represented by . If , the equation is impossible modulo four, so is odd. The integers and then have opposite parity, and therefore
Also , since otherwise ; hence
The Chinese remainder theorem gives the stronger conclusion
In particular,
as required.
Normalize the loop by
Choose a continuous lift satisfying
Because , the difference is an integer independent of the chosen lift. The winding number of a continuous closed path is
If is a lift of , then is a lift of
Therefore
Define
The strict inequality ensures that for every , while . Thus is a homotopy through closed loops in from to . By homotopy invariance of winding number,
Suppose for contradiction that has no zero in the closed disc. Then
is a homotopy through loops in . At it is , while at it is the constant loop with value . A constant loop has winding number zero, so homotopy invariance gives
contrary to the hypothesis. Hence
In Shannon-Fano coding, a symbol of probability is assigned length
and codewords of those lengths are chosen in lexicographic probability intervals; the Kraft inequality guarantees that a binary prefix code exists. Huffman coding repeatedly merges the two least probable current symbols, builds a binary tree from the resulting merges, and labels its two branches by zero and one. Reading from the root to each leaf gives an optimal prefix code.
The Shannon-Fano lengths are
One corresponding prefix-free assignment is
Its expected word length is
The Huffman coding merges are
For example, the resulting code may be
Its expected length is
The binary entropy is
The Shannon source coding theorem requires
for the standard Shannon construction, while every prefix code obeys the lower bound. Numerically,
Thus both codes satisfy the theorem, with the Huffman code closer to the entropy lower bound.
An alphabet is a finite nonempty set of symbols. A word over an alphabet is a finite sequence of symbols from , including the empty word ; the set of all words is . A formal language over is any subset .
A regular expression is defined recursively from , , and the individual symbols by the operations of finite union, concatenation, and Kleene star. Its language is defined by
There are only countably many regular expressions: each is a finite word over a finite collection of symbols and punctuation. On the other hand, for every nonempty finite alphabet, is countably infinite, so its power set is uncountable by the Cantor theorem. Thus there are uncountably many languages but only countably many languages denoted by regular expressions. Consequently
For log-likelihood , the score function and Fisher information matrix are
The Fisher scoring iteration replaces the observed Hessian in Newton's method by its expectation:
The weighted least squares objective is
Its gradient is
Since is positive diagonal and has full column rank, is positive definite. The unique stationary point is therefore the unique minimizer:
At a current value , put
and define the working response
Then the displayed formulas in the question can be written compactly as
and
Indeed, the th component of the latter is
which is precisely the stated score.
Substitution into the Fisher-scoring update gives
By part (b), this is the weighted least squares fit of the working response on . Both and are recomputed from the current fitted means after every update. Fisher scoring for a generalized linear model is therefore the iteratively reweighted least squares algorithm.
For drift and constant diffusion matrix , the Fokker-Planck equation is
Here
so
The drift is the linear vector field
The eigenvalues of its matrix are , so the origin is a stable spiral. The field rotates clockwise while contracting toward the origin:
Figure 1.
The drift vector field of a two-dimensional Ornstein-Uhlenbeck process
.
For this two-dimensional Ornstein-Uhlenbeck process, the covariance matrix
satisfies
Thus the stationary covariance solves the continuous Lyapunov equation
Write
Substitution gives
Solving,
Therefore
For , integration by parts gives
The boundary term vanishes, so the Gamma function recurrence is
Given any that is not a nonpositive integer, choose large enough that and define
The recurrence shows that definitions from different sufficiently large agree, so this gives the unique analytic continuation from the right half-plane. It is analytic except where a denominator factor vanishes, namely
These points are simple poles. More precisely, at ,
because one may write
and use .
Let each mass be and each spring constant be , with the denoting longitudinal displacements from equilibrium. The Lagrangian is
The inverse coordinate transformation is
Substitution gives
Thus the Euler-Lagrange equations separate into a symmetric pair,
and an antisymmetric pair,
The symmetric normal modes are:
  • , corresponding to and the translational frequency
  • , corresponding to and
For antisymmetric modes, the squared dimensionless frequencies are the eigenvalues of
namely . They give
and
In the original coordinates their mode shapes are respectively
and
The Hubble parameter is the fractional expansion rate
Here is the homogeneous energy density, records the sign of the spatial curvature of an FLRW universe, and is the fixed curvature length scale used with the dimensionless scale factor .
Energy-momentum conservation in a homogeneous expanding universe gives the continuity equation
Differentiate the Friedmann equation
Using and the continuity equation gives
Eliminating the curvature term with the Friedmann equation yields
Since , this is the Raychaudhuri equation
Under the strong energy condition , one has . Thus is concave, and for it lies below its tangent at the present time:
The right side vanishes at . A positive scale factor therefore cannot extend regularly to that time; it must reach the Big Bang singularity at some . Equivalently,
Using the Pauli matrices,
In a spherical coordinate system,
Since ,
The Pauli multiplication relations and give
Therefore the possible measurement outcomes, the eigenvalues of , are
The spectral projector for outcome is
For , the Born rule gives
The Born rule says that the probability of a projective-measurement outcome is the squared norm of the state projected onto the corresponding eigenspace. The basis vectors in the state whose second qubit is one are
They are mutually orthogonal, so
A binary block code of length is a subset . Its size is , and its minimum Hamming distance is
Thus an code consists of binary words of length whose distinct pairs differ in at least coordinates. When , every set of distinct words qualifies. Taking all of the binary vector space gives words, and no code can contain more words than its ambient space. Hence
Form the punctured code by deleting one fixed coordinate from every codeword. Two distinct original words differ in at least positions, so after one deletion they still differ and cannot coalesce. The new code therefore retains size , while every pairwise Hamming distance falls by at most one. It is an code with , and hence also an code in the minimum-distance-at-least convention. Therefore
Iterate the puncturing inequality from part (ii) times and then use part (i):
This is the binary Singleton bound:
Complete the square:
If is even, an integer can equal , giving the maximum . If is odd, every integer is at least from , giving the maximum . Thus
At coordinate , addition in gives exactly when . Therefore the number of ones in is exactly the number of coordinates in which the two words differ:
For column , let of the codewords have a one. A pair contributes a one in that column exactly when one word is chosen from those words and the other from the remaining . Hence column contains
ones among all pairwise sums. Part (i), summed over the columns, gives the upper bound
There are rows, one for each unordered pair of codewords. By part (ii), every row has weight equal to that pair's distance, which is at least . Therefore
Put . If is even, part (iii) gives
so
Because is even,
If is odd, part (iii) instead gives
Cancelling yields , and therefore
Since is an integer, the same desired upper bound follows. Thus the binary Plotkin bound is
A register machine has finitely many natural-number registers, a finite set of labelled states, and instructions that increment a register, conditionally decrement and branch according to whether a register is zero, or halt. A program is a finite sequence of such labelled instructions, and a configuration records the current instruction together with every current register value.
Given inputs, place them in designated input registers and initialize the remaining registers to zero. The machine computes a partial computable function when it halts with output in the output register exactly for and runs forever otherwise.
To encode a machine, encode every instruction by a natural number using effective encodings of its opcode, register number, and target labels. Encode the resulting finite sequence by a Gödel numbering, for example through iterated pairing or prime powers. Effective decoding gives an enumeration of machine programs, so the unary function computed by program code may be denoted .
Fix a register machine with inputs. By the permitted result, its complete configuration after steps,
is a recursive function of the inputs and time. The predicate saying that this configuration is halted is therefore recursive. Its halting time is the partial recursive function
where unbounded minimization is undefined when no halting time exists. Extracting the output register from a configuration is recursive, so
is partial recursive. Hence every partial computable function is partial recursive.
The function is not partial computable. It is defined on every input, so if a register machine with code computed it, then and in particular would be defined. The first clause in the definition would give
which is impossible. This is the usual diagonal argument behind the noncomputability of the diagonal halting set.
The function is also not partial computable. On every odd input it is defined, and
because the value in the halting case is . Thus a machine computing would decide diagonal halting for odd program indices simply by running and testing whether its output is zero.
That restricted problem remains undecidable. By the padding lemma, an arbitrary machine can effectively be replaced by an equivalent machine having an odd code—for example by adding unreachable instructions until the chosen effective encoding has the required parity. This gives a computable reduction from unrestricted diagonal halting to diagonal halting on odd indices. A decider obtained from would therefore decide the full diagonal halting problem, a contradiction. Hence
Kilometres is an ordinal categorical variable: its five levels have a meaningful order. Treating it as an ordinary factor would use four indicator variables and hence four unrelated regression coefficients. Converting the levels to numerical scores instead imposes a single linear trend across successive mileage bands. This is more parsimonious and gives greater precision when that trend is a reasonable approximation, although it also assumes that adjacent levels are equally spaced in their effect.
The graph is a profile likelihood for the parameter of a Box–Cox transformation. Its maximum is close to , and the displayed likelihood interval contains zero but excludes . Since gives a logarithmic transformation whereas leaves the response unchanged up to an affine transformation, the plot supports fitting
as the response in model2.
Because model2 uses a logarithmic transformation, the logarithm of the payment ratio is the difference of two predicted log payments. The cars have equal Brand and Bonus values and differ by one Kilometres level, so its fitted mean is the displayed mileage regression coefficient, .
For two independent future payments, the prediction interval must include both the standard error of and two independent residual errors. The estimated variance of the predicted log ratio is therefore
Using the residual degrees of freedom shown in the output, a 95% prediction interval for a ratio of log-normal responses is
With , this is approximately . The interval is wide because it predicts the ratio of two individual future payments; an interval for the ratio of their fitted mean responses would omit the term.
A suitable generalized linear model is a Gamma regression with logarithmic link:
with
The gamma distribution is appropriate for a positive, continuous, right-skewed payment, and its variance function allows the conditional variance to grow like the square of the conditional mean instead of assuming constant variance. The logarithmic link function also guarantees positive fitted means and represents covariate effects multiplicatively, which accords with the Box–Cox transformation evidence for a logarithmic scale.
Put with . The chain rule gives
and hence
After substitution and division by , the ordinary differential equation becomes
Comparison with the Gauss hypergeometric equation gives, up to interchanging and ,
At and , the coefficient of has at most a simple pole and that of has at most a double pole, so both are regular singular points. The regular singular point at infinity criterion gives the same conclusion at infinity. The corresponding Papperitz symbol is
Indeed, the exponent pairs are at zero, at one, and at infinity; their sum also satisfies the Fuchs relation.
The solution of with and is . Near , the map has the local inverse , so this solution is analytic in , corresponds to exponent zero at , and has value one there. Uniqueness of the normalized local solution of the Gauss hypergeometric equation therefore gives the hypergeometric cosine identity
or, when on the chosen local branch,
Since , the second local hypergeometric solution is
Under , it must be a constant multiple of the independent elementary solution . As , both and are asymptotic to one another, while . Matching the normalized hypergeometric factor, whose value at zero is one, gives
Consequently the hypergeometric sine identity is
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