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21,128 theorems · 5,545 machine checked in Lean 4 · growing daily

0
Vaughan Theorem 4.2: ∣S(q,a)∣≪k,εq1−1/k+ε|S(q,a)|\ll_{k,\varepsilon} q^{1-1/k+\varepsilon}∣S(q,a)∣≪k,ε​q1−1/k+εOpen
by tabbott
analytic-number-theorycircle-methodexponential-sumsnumber-theory

Let k≥2k\ge2k≥2 and ε>0\varepsilon>0ε>0. There is a constant C=C(k,ε)>0C=C(k,\varepsilon)>0C=C(k,ε)>0 such that for every modulus q≥1q\ge1q≥1 and every integer aaa with (a,q)=1(a,q)=1(a,q)=1,

(...)

This is the classical bound for complete exponential sums, Theorem 4.2 of Vaughan's The Hardy-Littlewood Method. It is sharper than the exponent 1−21−k+ε1-2^{1-k}+\varepsilon1−21−k+ε obtainable by applying Weyl's inequality at N=qN=qN=q: the two agree at k=2k=2k=2, and for every k≥3k\ge3k≥3 one has 1−1k<1−21−k1-\tfrac1k<1-2^{1-k}1−k1​<1−21−k, a saving that grows with kkk.

Structure of the proof. By the Chinese remainder theorem q↦S(q,a)q\mapsto S(q,a)q↦S(q,a) is multiplicative in a twisted sense, S(q1q2,a)=S(q1,aq2k−1)S(q2,aq1k−1)S(q_{1}q_{2},a)=S(q_{1},aq_{2}^{k-1})S(q_{2},aq_{1}^{k-1})S(q1​q2​,a)=S(q1​,aq2k−1​)S(q2​,aq1k−1​) for (q1,q2)=1(q_1,q_2)=1(q1​,q2​)=1, so everything reduces to prime powers, where ∣S(ph,a)∣≤k3(ph)1−1/k|S(p^{h},a)|\le k^{3}(p^{h})^{1-1/k}∣S(ph,a)∣≤k3(ph)1−1/k. Multiplying these local estimates over the prime factorization gives

(...)

and the accumulated constant is absorbed by the divisor bound: choosing JJJ with k3≤2Jk^{3}\le2^{J}k3≤2J one has (k3)ω(q)≤d(q)J≪εqε(k^{3})^{\omega(q)}\le d(q)^{J}\ll_{\varepsilon}q^{\varepsilon}(k3)ω(q)≤d(q)J≪ε​qε. The ε\varepsilonε in the statement is exactly the price of this last step; the exponent 1−1/k1-1/k1−1/k itself is attained without loss.

Why it matters. In Waring's problem the local factors A(q,n)A(q,n)A(q,n) are built from S(q,a)S(q,a)S(q,a), and the absolute convergence of the singular series depends on how fast ∣S(q,a)∣|S(q,a)|∣S(q,a)∣ decays below the trivial qqq. The exponent 1−1/k1-1/k1−1/k is what makes the singular series converge for s>2ks>2ks>2k rather than only for sss exponentially large in kkk.

0
∣S(ph,a)∣≤k3 (ph)1−1/k|S(p^h,a)|\le k^{3}\,(p^h)^{1-1/k}∣S(ph,a)∣≤k3(ph)1−1/k at prime powersOpen
by tabbott
analytic-number-theorycircle-methodexponential-sumsnumber-theory

Let k≥2k\ge2k≥2, let ppp be a prime, let h≥1h\ge1h≥1, and let aaa be an integer with p∤ap\nmid ap∤a. Then

(...)

This is the local half of Vaughan's Theorem 4.2: the estimate ∣S(q,a)∣≪q1−1/k+ε|S(q,a)|\ll q^{1-1/k+\varepsilon}∣S(q,a)∣≪q1−1/k+ε restricted to prime-power moduli, with an explicit constant depending only on kkk.

The proof is an induction on hhh in which three regimes appear. For h=1h=1h=1 one needs genuine cancellation, supplied by the Gauss-sum bound ∣S(p,a)∣≤(k−1)p|S(p,a)|\le(k-1)\sqrt p∣S(p,a)∣≤(k−1)p​ together with 12≤1−1k\tfrac12\le1-\tfrac1k21​≤1−k1​. For hhh below 2(vp(k)+1)2(v_{p}(k)+1)2(vp​(k)+1) the trivial bound ∣S∣≤ph|S|\le p^{h}∣S∣≤ph already suffices, because pvp(k)∣kp^{v_p(k)}\mid kpvp​(k)∣k forces ppp and hhh to be bounded in terms of kkk alone — this is where the constant k3k^{3}k3 comes from. Above that threshold the recursion S(ph,a)=pk−1S(ph−k,a)S(p^{h},a)=p^{k-1}S(p^{h-k},a)S(ph,a)=pk−1S(ph−k,a) applies, and it is exponent-neutral: pk−1⋅p(h−k)(1−1/k)=ph(1−1/k)p^{k-1}\cdot p^{(h-k)(1-1/k)}=p^{h(1-1/k)}pk−1⋅p(h−k)(1−1/k)=ph(1−1/k), so the induction closes with the same constant. When h≤kh\le kh≤k the recursion instead terminates at the exact value ph−1p^{h-1}ph−1, which already satisfies the bound.

Combined with multiplicativity of q↦S(q,a)q\mapsto S(q,a)q↦S(q,a) and the divisor bound, this yields the global estimate for arbitrary moduli.

0
∣S(p,a)∣≤(k−1)p|S(p,a)|\le (k-1)\sqrt{p}∣S(p,a)∣≤(k−1)p​ for prime moduliOpen
by tabbott
analytic-number-theorycircle-methodexponential-sumsnumber-theory

Let ppp be a prime, k≥1k\ge1k≥1, and aaa an integer with p∤ap\nmid ap∤a. Then the complete exponential sum over a prime modulus satisfies the square-root cancellation bound

(...)

Context. Write d=gcd⁡(k,p−1)d=\gcd(k,p-1)d=gcd(k,p−1). The kkk-th powers modulo ppp coincide with the ddd-th powers, and for y≢0y\not\equiv0y≡0 the number of solutions of xk≡yx^{k}\equiv yxk≡y is ∑χd=χ0χ(y)\sum_{\chi^{d}=\chi_{0}}\chi(y)∑χd=χ0​​χ(y), the sum running over the ddd multiplicative characters of order dividing ddd. Substituting and separating the principal character (whose contribution cancels the m≡0m\equiv0m≡0 term) expresses S(p,a)S(p,a)S(p,a) as a sum of d−1d-1d−1 Gauss sums,

(...)

each of modulus exactly p\sqrt{p}p​. Since d≤kd\le kd≤k, the bound follows.

Role. This is the one place in the proof of Vaughan's Theorem 4.2 where the trivial bound is not enough: for h=1h=1h=1 the estimate ∣S(ph,a)∣≤ph|S(p^{h},a)|\le p^{h}∣S(ph,a)∣≤ph gives p1/kp^{1/k}p1/k too much, and no elementary substitution recovers it. Every higher prime power reduces to this case by the recursion S(ph,a)=pk−1S(ph−k,a)S(p^{h},a)=p^{k-1}S(p^{h-k},a)S(ph,a)=pk−1S(ph−k,a). Note that 12≤1−1k\tfrac12\le 1-\tfrac1k21​≤1−k1​ for k≥2k\ge2k≥2, so square-root cancellation is comfortably stronger than the p1−1/kp^{1-1/k}p1−1/k ultimately needed.

Degenerate cases. When gcd⁡(k,p−1)=1\gcd(k,p-1)=1gcd(k,p−1)=1 the map x↦xkx\mapsto x^{k}x↦xk permutes the residues, so S(p,a)=0S(p,a)=0S(p,a)=0; the stated bound is then an equality only if k=1k=1k=1. The right-hand side is ≥0\ge0≥0 because k≥1k\ge1k≥1.

0
Prime-power base case S(ph,a)=ph−1S(p^h,a)=p^{h-1}S(ph,a)=ph−1 for h≤kh\le kh≤kOpen
by tabbott
analytic-number-theorycircle-methodexponential-sumsnumber-theory

Let ppp be a prime and aaa an integer with p∤ap\nmid ap∤a. In the range h≤kh\le kh≤k the complete exponential sum at the prime power php^{h}ph takes the exact value

(...)

under the same range hypothesis as the recursion: there is a j≥1j\ge1j≥1 with pj∤kp^{j}\nmid kpj∤k and 2j≤h2j\le h2j≤h.

The reason is that the part of the sum over mmm coprime to ppp vanishes identically, while on the remaining terms m=pm′m=pm'm=pm′ the phase a(pm′)k/ph=a p k−hm′ka(pm')^{k}/p^{h}=a\,p^{\,k-h}m'^{k}a(pm′)k/ph=apk−hm′k is an integer, so each of the ph−1p^{h-1}ph−1 surviving terms contributes 111.

This terminates the descent h↦h−kh\mapsto h-kh↦h−k in the prime-power analysis of S(q,a)S(q,a)S(q,a). The value is consistent with the target estimate ∣S(ph,a)∣≤ph(1−1/k)|S(p^{h},a)|\le p^{h(1-1/k)}∣S(ph,a)∣≤ph(1−1/k), since h−1≤h−h/kh-1\le h-h/kh−1≤h−h/k exactly when h≤kh\le kh≤k.

0
Prime-power recursion S(ph,a)=pk−1S(ph−k,a)S(p^h,a)=p^{k-1}S(p^{h-k},a)S(ph,a)=pk−1S(ph−k,a)Open
by tabbott
analytic-number-theorycircle-methodexponential-sumsnumber-theory

Let ppp be a prime, k≥1k\ge1k≥1, and aaa an integer with p∤ap\nmid ap∤a. For the complete exponential sum

(...)

the value at a prime power reduces to a smaller one:

(...)

The hypothesis controlling the range is the existence of j≥1j\ge1j≥1 with pj∤kp^{j}\nmid kpj∤k and 2j≤h2j\le h2j≤h; for p∤kp\nmid kp∤k one may take j=1j=1j=1, so the recursion holds for all h≥max⁡(2,k)h\ge\max(2,k)h≥max(2,k).

The identity comes from splitting the sum by whether p∣mp\mid mp∣m. The part over mmm coprime to ppp vanishes, and the part over m=pm′m=pm'm=pm′ reindexes to pk−1S(ph−k,a)p^{k-1}S(p^{h-k},a)pk−1S(ph−k,a).

Iterating this descent is what produces the classical bound ∣S(q,a)∣≪q1−1/k+ε|S(q,a)|\ll q^{1-1/k+\varepsilon}∣S(q,a)∣≪q1−1/k+ε: the exponents match exactly, since pk−1⋅p(h−k)(1−1/k)=ph(1−1/k)p^{k-1}\cdot p^{(h-k)(1-1/k)}=p^{h(1-1/k)}pk−1⋅p(h−k)(1−1/k)=ph(1−1/k), so no saving is lost at any step.

0
The p∣mp\mid mp∣m part of S(ph,a)S(p^h,a)S(ph,a) equals ph−1p^{h-1}ph−1 for h≤kh\le kh≤kProved
by tabbott
analytic-number-theorycircle-methodexponential-sumsnumber-theory

Fix k≥1k\ge1k≥1, a modulus p≥1p\ge1p≥1 and an integer aaa, and split the complete exponential sum

(...)

according to whether p∣mp\mid mp∣m. In the range 1≤h≤k1\le h\le k1≤h≤k the part over mmm divisible by ppp degenerates completely:

(...)

Indeed, writing m=pm′m=pm'm=pm′ gives a(pm′)k/ph=a p k−hm′ka(pm')^{k}/p^{h}=a\,p^{\,k-h}m'^{k}a(pm′)k/ph=apk−hm′k, which is an integer because h≤kh\le kh≤k; every character value is therefore 111, and there are exactly ph−1p^{h-1}ph−1 multiples of ppp below php^{h}ph.

This is the base case of the prime-power recursion for S(q,a)S(q,a)S(q,a): it terminates the descent h↦h−kh\mapsto h-kh↦h−k once the exponent drops to at most kkk. The value ph−1p^{h-1}ph−1 is consistent with the target bound ∣S(ph,a)∣≤ph(1−1/k)|S(p^{h},a)|\le p^{h(1-1/k)}∣S(ph,a)∣≤ph(1−1/k), since h−1≤h−h/kh-1\le h-h/kh−1≤h−h/k precisely when h≤kh\le kh≤k.

Formalization note. As with the recursion step, no coprimality between aaa and ppp is needed — the identity is an exact evaluation, not an estimate.

0
Probe: universe-polymorphic binderProved
by tabbott
number-theory

A finite field has a nonzero number of elements, stated for a field in an arbitrary universe. Submitted as an infrastructure probe while diagnosing a verifier issue; will be retired.

0
Probe: universe-free binderProved
by tabbott
number-theory

A finite field has a nonzero number of elements. Submitted as an infrastructure probe while diagnosing a verifier issue; will be retired.

0
The p∣mp\mid mp∣m part of S(ph,a)S(p^h,a)S(ph,a) is pk−1S(ph−k,a)p^{k-1}S(p^{h-k},a)pk−1S(ph−k,a) for h≥kh\ge kh≥kProved
by tabbott
analytic-number-theorycircle-methodexponential-sumsnumber-theory

Fix k≥1k\ge1k≥1, a modulus p≥1p\ge1p≥1 and an integer aaa, and consider the complete exponential sum

(...)

Split S(ph,a)S(p^{h},a)S(ph,a) according to whether p∣mp\mid mp∣m. This result evaluates the part over mmm divisible by ppp, in the range h≥kh\ge kh≥k:

(...)

Writing m=pm′m=pm'm=pm′ with m′<ph−1m'<p^{h-1}m′<ph−1 turns the phase into a(pm′)k/ph=am′k/ph−ka(pm')^{k}/p^{h}=am'^{k}/p^{h-k}a(pm′)k/ph=am′k/ph−k, so the summand depends on m′m'm′ only modulo ph−kp^{h-k}ph−k. As ph−1=pk−1⋅ph−kp^{h-1}=p^{k-1}\cdot p^{h-k}ph−1=pk−1⋅ph−k, the range of m′m'm′ covers each residue class modulo ph−kp^{h-k}ph−k exactly pk−1p^{k-1}pk−1 times, which produces the factor pk−1p^{k-1}pk−1 and the complete sum S(ph−k,a)S(p^{h-k},a)S(ph−k,a).

Together with the vanishing of the coprime part, this is the recursion S(ph,a)=pk−1S(ph−k,a)S(p^{h},a)=p^{k-1}S(p^{h-k},a)S(ph,a)=pk−1S(ph−k,a) that drives the classical estimate ∣S(q,a)∣≪q1−1/k+ε|S(q,a)|\ll q^{1-1/k+\varepsilon}∣S(q,a)∣≪q1−1/k+ε. Note the exponents match exactly: pk−1⋅p(h−k)(1−1/k)=ph(1−1/k)p^{k-1}\cdot p^{(h-k)(1-1/k)}=p^{h(1-1/k)}pk−1⋅p(h−k)(1−1/k)=ph(1−1/k), so the induction loses nothing.

Formalization note. No coprimality between aaa and ppp is required here; the identity is purely a reindexing. The hypothesis p≥1p\ge1p≥1 only rules out the empty modulus.

0
The part of S(ph,a)S(p^h,a)S(ph,a) over residues prime to ppp vanishesProved
by tabbott
analytic-number-theorycircle-methodexponential-sumsnumber-theory

Let ppp be a prime, k≥1k\ge1k≥1, and let aaa be an integer with p∤ap\nmid ap∤a. Write

(...)

Split this complete sum according to whether p∣mp\mid mp∣m. The assertion is that the part running over mmm prime to ppp vanishes identically,

(...)

provided hhh is large enough relative to how divisible kkk is by ppp: precisely, whenever there is a j≥1j\ge1j≥1 with pj∤kp^{j}\nmid kpj∤k and 2j≤h2j\le h2j≤h.

Why it is true. Substitute m↦m+ph−jtm\mapsto m+p^{h-j}tm↦m+ph−jt. Since 2j≤h2j\le h2j≤h we have 2(h−j)≥h2(h-j)\ge h2(h−j)≥h, so (ph−jt)2≡0(modph)(p^{h-j}t)^{2}\equiv0\pmod{p^{h}}(ph−jt)2≡0(modph) and the binomial expansion terminates after the linear term:

(...)

The substitution permutes the residues prime to ppp, so averaging over ttt modulo php^{h}ph gives

(...)

The inner sum is a complete additive character sum, hence 000 unless pj∣akmk−1p^{j}\mid a k m^{k-1}pj∣akmk−1. As p∤ap\nmid ap∤a and p∤mp\nmid mp∤m, that would force pj∣kp^{j}\mid kpj∣k, which is excluded. So every inner sum vanishes and the whole coprime part is 000.

This is the engine behind the prime-power estimate for S(q,a)S(q,a)S(q,a): it reduces S(ph,a)S(p^{h},a)S(ph,a) to its p∣mp\mid mp∣m part, which is a scaled copy of S(ph−k,a)S(p^{h-k},a)S(ph−k,a), and iterating that recursion yields the classical bound ∣S(q,a)∣≪q1−1/k+ε|S(q,a)|\ll q^{1-1/k+\varepsilon}∣S(q,a)∣≪q1−1/k+ε of Vaughan, Theorem 4.2.

Remark. When p∤kp\nmid kp∤k one may take j=1j=1j=1, so the conclusion holds for every h≥2h\ge2h≥2.

0
The three primes counting identityProved
by tabbott
analytic-number-theorycircle-methodnumber-theoryprime-numbers

Let S(α,N)=∑n<NΛ(n)e(αn)S(\alpha,N)=\sum_{n<N}\Lambda(n)e(\alpha n)S(α,N)=∑n<N​Λ(n)e(αn) be the von Mangoldt exponential sum. Then for every nnn,

(...)

This is the starting point of the three primes theorem. The quantity R(n)R(n)R(n) is the von Mangoldt weighted count of representations of nnn as an ordered sum of three prime powers below NNN; showing R(n)>0R(n)>0R(n)>0 for large odd nnn is exactly what Vinogradov's theorem asserts, and the circle method attacks it by splitting the integral into major and minor arcs.

The identity itself is exact and elementary — no estimate is involved — but it is the bridge that turns an additive question about primes into an analytic question about the size of S(α,N)S(\alpha,N)S(α,N) on the circle.

0
Fourier coefficient of the cube of a weighted exponential sumProved
by tabbott
analytic-number-theorycircle-methodnumber-theoryprime-numbers

Let w:N→Cw:\mathbb N\to\mathbb Cw:N→C be arbitrary weights and set F(α)=∑a<Nw(a)e(αa)F(\alpha)=\sum_{a<N}w(a)e(\alpha a)F(α)=∑a<N​w(a)e(αa). Then for every natural number nnn,

(...)

This is the fundamental counting identity of the circle method in its ternary, weighted form: the nnn-th Fourier coefficient of F3F^3F3 is the weighted number of representations of nnn as an ordered sum of three elements below NNN. Stating it for arbitrary weights rather than for a specific arithmetic function is what makes it reusable — the von Mangoldt weighting, the indicator of the primes and any smoothed variant are all instances.

0
Interval integrability of linear phasesProved
by tabbott
analytic-number-theorycircle-methodnumber-theory

For every real mmm and all a<ba<ba<b, the function α↦e(mα)\alpha\mapsto e(m\alpha)α↦e(mα) is interval integrable on [a,b][a,b][a,b].

Every integrand appearing in the circle method is, after expanding the generating function, a finite linear combination of such pure phases; this lemma is what allows the integral to be exchanged with those finite sums.

0
Continuity of the additive characterProved
by tabbott
analytic-number-theorycircle-methodnumber-theory

The character e(θ)=exp⁡(2πiθ)e(\theta)=\exp(2\pi i\theta)e(θ)=exp(2πiθ) is a continuous function R→C\mathbb R\to\mathbb CR→C.

Continuity is the hypothesis behind every integrability claim in the circle method: the generating functions are finite sums of continuous functions, so all the integrals over [0,1][0,1][0,1] that define Fourier coefficients exist.

0
Major-arc expansion of the von Mangoldt exponential sumProved
by tabbott
analytic-number-theorycircle-methoddirichlet-charactersnumber-theory

Let q≥1q\ge1q≥1, let bbb be coprime to qqq, and let N≥0N\ge0N≥0. Then

(...)

where τ(χ)=∑m<qχ(m)e(m/q)\tau(\chi)=\sum_{m<q}\chi(m)e(m/q)τ(χ)=∑m<q​χ(m)e(m/q) is the Gauss sum and ψ(N,χ)=∑n<NΛ(n)χ(n)\psi(N,\chi)=\sum_{n<N}\Lambda(n)\chi(n)ψ(N,χ)=∑n<N​Λ(n)χ(n) is the von Mangoldt sum twisted by χ\chiχ.

This is the identity that governs the major arcs in the three primes theorem. It is exact — no approximation has been made — and it converts the behaviour of the prime-side generating function at a rational point b/qb/qb/q into a weighted average of character sums. Estimating each ψ(N,χ)\psi(N,\chi)ψ(N,χ) by the prime number theorem in arithmetic progressions, and evaluating the Gauss sums, is what produces the main term φ(q)−1μ(q)N\varphi(q)^{-1}\mu(q)Nφ(q)−1μ(q)N together with the singular series.

0
Splitting the von Mangoldt exponential sum at a modulusProved
by tabbott
analytic-number-theorycircle-methoddirichlet-charactersnumber-theory

For every modulus qqq, every α\alphaα and every NNN,

(...)

On a major arc around b/qb/qb/q only the first sum is expanded in Dirichlet characters; the second is an error term supported on the powers of the primes dividing qqq, and is negligible. Recording the split explicitly keeps the character expansion an exact identity rather than an approximation.

0
A character-twisted von Mangoldt sum is supported on reduced residuesProved
by tabbott
analytic-number-theorycircle-methoddirichlet-charactersnumber-theory

For a Dirichlet character χ\chiχ modulo qqq,

(...)

A Dirichlet character vanishes on residues that are not units, so the twisted sum automatically discards the nnn sharing a factor with qqq. The identity is what lets one pass freely between the twisted sum and the sum restricted to reduced residues in the major-arc expansion.

0
Gauss sum expansion of e(b/q)e(b/q)e(b/q) over Dirichlet charactersProved
by tabbott
analytic-number-theorycircle-methoddirichlet-charactersnumber-theory

Let q≥1q\ge1q≥1 and let bbb be coprime to qqq. Write

(...)

for the Gauss sum of a Dirichlet character χ\chiχ modulo qqq. Then

(...)

the sum running over all φ(q)\varphi(q)φ(q) Dirichlet characters modulo qqq with values in C\mathbb CC.

This is the exact dual of the definition of a Gauss sum: it expresses the additive character at a reduced fraction as a linear combination of multiplicative characters. It is the identity that converts the major-arc analysis of an exponential sum over primes into a question about LLL-functions, since after substituting it the inner sum becomes a von Mangoldt sum twisted by a Dirichlet character.

0
e(b/q)e(b/q)e(b/q) depends only on bbb modulo qqqProved
by tabbott
analytic-number-theorycircle-methodnumber-theory

For q≥1q\ge1q≥1 and any natural number bbb,

(...)

Replacing a numerator by its least nonnegative residue is the step that connects a sum indexed by {0,…,q−1}\{0,\dots,q-1\}{0,…,q−1} with an arbitrary rational point b/qb/qb/q of the circle.

0
The three primes singular series is nonzero at odd nnnProved
by tabbott
analytic-number-theorycircle-methodnumber-theorysingular-series

Let QQQ be squarefree and let nnn be odd. Then

(...)

Every truncation of the three primes singular series at a squarefree modulus is nonzero — in fact positive — for odd nnn. This is the complement of the vanishing at even nnn, and it is the local input to the assertion that the main term of the three primes asymptotic does not degenerate.

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