![Let Qp,q(t)āā¤[t] be Sharipov's even monic degree-10 second cuboid polynomial, with coprime positive integers pā q. We prove that Qp,q(t) is irreducible over ā, and hence over ā¤. More generally, the normalized associated quintic Pā(x) and its composition Pā(t²) are irreducible over ā for every sāāā{0,±1}. The proof reduces linear and quadratic factors to rational points and horizontal conjugate pairs on one fixed genus-2 curve. A certified rank upper bound for its Jacobian, together with an exact divisor calculation, gives a rank-one annihilating differential at the prime 3. For the quadratic-factor case, the symmetric coordinates of a horizontal pair lie on an explicit double cover of an elliptic quartic. All rational affine points on this model are 3-adically integral and reduce to six smooth residue classes. The pulled-back differential is a unit in each class, proving that six displayed points form the complete list. Their coordinates exclude every admissible parameter. A negative r](https://pbs.twimg.com/media/HVD9RX6X0AAuFHR.png?name=small&format=webp)
ALT Let Qp,q(t)āā¤[t] be Sharipov's even monic degree-10 second cuboid polynomial, with coprime positive integers pā q. We prove that Qp,q(t) is irreducible over ā, and hence over ā¤. More generally, the normalized associated quintic Pā(x) and its composition Pā(t²) are irreducible over ā for every sāāā{0,±1}. The proof reduces linear and quadratic factors to rational points and horizontal conjugate pairs on one fixed genus-2 curve. A certified rank upper bound for its Jacobian, together with an exact divisor calculation, gives a rank-one annihilating differential at the prime 3. For the quadratic-factor case, the symmetric coordinates of a horizontal pair lie on an explicit double cover of an elliptic quartic. All rational affine points on this model are 3-adically integral and reduce to six smooth residue classes. The pulled-back differential is a unit in each class, proving that six displayed points form the complete list. Their coordinates exclude every admissible parameter. A negative r

ALT In the present paper, we investigate geometric properties of a Riemannian submersion for which the total manifold is endowed with hyperbolic and almost hyperbolic Ricci solitons. We establish conditions under which the fibers of the submersion admit hyperbolic and almost hyperbolic Ricci solitons. Further, we derive necessary conditions for the base manifold to be an Einstein and a hyperbolic Ricci soliton. Also, we determine the scalar curvature associated with the fibers and the base manifold. Moreover, when the total space admits an almost hyperbolic Ricci soliton with a torse-forming potential vector field, we obtain conditions ensuring that the extrinsic vertical and horizontal distributions are almost generalized quasi-Einstein. We also obtain necessary conditions for the fibers and base manifold to be an Einstein and almost generalized quasi-Einstein manifold. Finally, examples are included to illustrate the existence of hyperbolic and almost hyperbolic Ricci solitons in Riemann

ALT The secondary zeta function is defined by Z(s)=āγ>ā¹āγā, where tfrac12+iγ runs over the non-trivial zeros of the Riemann zeta function with positive ordinate, and the Riemann hypothesis is assumed throughout. In this article, we derive convergent integral representations of Z(s) at positive even and odd integer argument, expressed through a differential operator acting on the logarithm of the Riemann ξ-function. Define L(x)=log(ξ(x+tfrac12)/ξ(tfrac12)), ā°=xįµādā, Dā=ā°āā±¼āāįµ(ā°-2j). Then, for kā„1, Z(2k)=(-1)įµ/2įµ(k-1)!ā«āāDā L(x)/x²įµāŗĀ¹ dx and Z(2k+1)=(-1)įµ/Ļ (2k-1)!!ā«āāDā L(x)/x²įµāŗĀ² dx. In the last part, we write these formulas out explicitly for Z(k), 2⤠k⤠7, both in terms of L(x) and in terms of ξ(x+tfrac12) for reference. We also derive a limit formula for γā, the ordinate of the first nontrivial zero, and demonstrate its convergence numerically.

ALT Generalized Pellet's theorem is extended to analytic matrix-valued functions using Descartes' rule of signs for infinite series. Cauchy's estimate is incorporated to allow numerical computation of the bounds. To address the issue that Pellet's theorem and its generalizations may not always guarantee the existence of bounds, for the case of matrix size one, we employ the Dandelin- Lobachevsky-Graeffe method, which ensures the existence of the bounds for the roots and further improves them as the order of the transform increases. Without the need for any a priori information on the function, these theorems allow us to compute mathematically verified bounds for the roots in a certain region using an interval arithmetic implementation of the function. Numerical examples and an implementation are provided to illustrate the effectiveness of the proposed method.

ALT We present an elementary but powerful method for proving that a two-variable equation has no integer solutions. The method produces quadratic identities which every integer solution must satisfy. Once these identities are established, a standard quadratic reciprocity argument finishes the proof. We illustrate the power of the method by resolving 25 out of 30 two-variable equations of size up to 34 for which the problem of integer solubility remained open. We also resolve the remaining 5 equations by deeper methods, and further determine the integer solubility of all two-variable equations of size up to 35 and of length up to 12, with two exceptions. Before this work, there were 211 equations in this category that resisted the previously known methods, and we proved that 209 of them have no integer solutions, with all proofs formalized in Lean. In addition, we show that our method can be used to solve certain two-variable equations whose integer solution set is non-empty.
![A continuous shape parameter enters both a radial density and the normalization of its transform coefficients. This coupling allows changes in shape to be compensated by changes in scale and exponential tilt. We study the coefficients bā=eįµ E[Yįµ ]/[k!(d)ā ] for densities proportional to yā½d-1) exp(-αyq+e̲tay), with known integer q>=2, d,α>0, and unrestricted real a,e̲ta. For q=2, the first four coefficients determine all parameters globally, whereas three coefficients leave an analytic curve of solutions. We characterize the exact image of the two shape ratios and prove that two alternating corners decide whether an entire coefficient box is realizable and give its exact shape range. For every fixed q, the first q(q+1) coefficients give global identification and an everywhere full-rank map. A finite-difference criterion yields generic identification from 2q+1 coefficients, including every zero-tilt model against the full tilted family. For q=3, an exact rational certificate constructs](https://pbs.twimg.com/media/HUrS6CLXMAAJ96F.png?name=small&format=webp)
ALT A continuous shape parameter enters both a radial density and the normalization of its transform coefficients. This coupling allows changes in shape to be compensated by changes in scale and exponential tilt. We study the coefficients bā=eįµ E[Yįµ ]/[k!(d)ā ] for densities proportional to yā½d-1) exp(-αyq+e̲tay), with known integer q>=2, d,α>0, and unrestricted real a,e̲ta. For q=2, the first four coefficients determine all parameters globally, whereas three coefficients leave an analytic curve of solutions. We characterize the exact image of the two shape ratios and prove that two alternating corners decide whether an entire coefficient box is realizable and give its exact shape range. For every fixed q, the first q(q+1) coefficients give global identification and an everywhere full-rank map. A finite-difference criterion yields generic identification from 2q+1 coefficients, including every zero-tilt model against the full tilted family. For q=3, an exact rational certificate constructs

ALT A set of m distinct positive integers is called a Diophantine m-tuple if the product of any two distinct elements, increased by one, is a perfect square. A Diophantine quadruple {a,b,c,d} with a<b<c<d is called regular if d=a+b+c+2abc+2ā((ab+1)(ac+1)(bc+1)). We prove that every irregular Diophantine quadruple satisfies c<10³³⸠and d<10¹ā°Ā²ā“.

ALT The 2026 measles resurgence in Bangladesh motivates a spatial modelling framework that accounts for heterogeneous local transmission, vaccination activity, and interdivisional connectivity. We formulate a multipatch susceptible-vaccinated-infectious-recovered model for the eight administrative divisions of Bangladesh. Division-specific parameters are estimated from reported measles cases and smoothed vaccination data using bounded nonlinear least squares, with uncertainty quantified through 1000 parametric bootstrap replicates. The fitted divisional systems are then connected through compartment-specific movement and cross-patch infection coefficients adjusted for connectivity and the source division's relative reproduction number. The fitted model captures the main division-specific epidemic patterns. Estimated local reproduction numbers range from 1.1386 in Khulna (95% CI:0.5703ā1.3834) to 4.3491 in Dhaka (95% CI: 1.4449ā5.6307), while Chattogram also exhibits high transmission poten
![Let K be an imaginary quadratic field with fundamental discriminant D=-5n, where n>0 is odd, and cyclic ideal class group Cl(K)=langle granglesimeq CāM. Assume that the ramified prime class above 5 is the unique involution g²M. For the Kronecker eta invariant F(A)=|Ī·(z_A)|²/āa_A, where z_A and a_A arise from a positive definite quadratic form representing the ideal class A, we show that the logarithms of the mirror ratios R_j=F(g²M-j)/F(g^j), 0⤠j<M, are related by an explicit discrete cosine transform to the odd class-character Hecke L(1)-values. A single level-5 generalized-Weber orbit realizes all of these mirrors. Combining Fourier nonvanishing, lower-power Weber class invariants and a ray-class cancellation argument, we prove mathbbQ(R_j)=H^langlecrangle, R_j^{ϲM}=R_j^-1, mathbbQ(R_j+R_j^-1)=H^{langlec,ϲMrangle}. Here H is the Hilbert class field, c denotes complex conjugation, and Ļ corresponds to g under the Artin map. Consequently [mathbbQ(R_j):mathbbQ]=4M, [mathbbQ(R_j+R_j^-](https://pbs.twimg.com/media/HUqz8m8W8AELJcI.png?name=small&format=webp)
ALT Let K be an imaginary quadratic field with fundamental discriminant D=-5n, where n>0 is odd, and cyclic ideal class group Cl(K)=langle granglesimeq CāM. Assume that the ramified prime class above 5 is the unique involution g²M. For the Kronecker eta invariant F(A)=|Ī·(z_A)|²/āa_A, where z_A and a_A arise from a positive definite quadratic form representing the ideal class A, we show that the logarithms of the mirror ratios R_j=F(g²M-j)/F(g^j), 0⤠j<M, are related by an explicit discrete cosine transform to the odd class-character Hecke L(1)-values. A single level-5 generalized-Weber orbit realizes all of these mirrors. Combining Fourier nonvanishing, lower-power Weber class invariants and a ray-class cancellation argument, we prove mathbbQ(R_j)=H^langlecrangle, R_j^{ϲM}=R_j^-1, mathbbQ(R_j+R_j^-1)=H^{langlec,ϲMrangle}. Here H is the Hilbert class field, c denotes complex conjugation, and Ļ corresponds to g under the Artin map. Consequently [mathbbQ(R_j):mathbbQ]=4M, [mathbbQ(R_j+R_j^-

ALT For an odd prime p, we study the change in matrix order under lifting from Z/pįµ Z to Z/pā½k+1) Z. The first variation of the order defect is an affine translate of a cyclic adjoint transfer on slā(Fā). We classify the full-order transfer for every q in GLā(Fā): its rank is 3 for scalar elements, 1 for nonscalar semisimple elements, 1 for nonscalar Jordan elements when p = 3, and 0 for nonscalar Jordan elements when p > 3. For a Jordan element q = lambda(I + U), U² = 0 and U!=0, the vanishing first-order transfer for p > 3 admits an exact higher-order refinement. Writing d = (p - 1)/2, the full-order perturbation has depth d when tr(UX)!=0, depth p - 1 when tr(UX) = 0 and X is not in the span of U, and vanishes identically for X in the span of U. For p = 3, among the 27 lifts of a nonscalar order-preserving parent with determinant fixed to +1 or -1, exactly 9 preserve its order and 18 triple it; after the first increase, every further lift triples the order. We also give a scalar obstruc

ALT We give a self-contained derivation of the closed form of the power sums Sā(n)=āįµ¢āāāæ(aā+(i-1)d)įµ in which the Bernoulli numbers enter as constants of integration rather than as prescribed coefficients. The derivation rests on an elementary fact: a sum whose terms are polynomial in the index is the restriction to the integers of a unique polynomial, which satisfies the defining difference equation identically and may therefore be differentiated and integrated exactly. Differentiating lowers the power by one; integrating back introduces a single constant, equal to the slope Sā'(0) of the polynomial at the origin and fixed by the value Sā(1)=aāįµ. This yields a closed form for Sā(n) in terms of the constants and a recurrence that determines them, obtained without induction on the exponent and without generating functions. With the Bernoulli numbers defined by their classical recurrence, we identify the constants as dįµBā(aā/d); the progression starting at 0 reproduces that recurrence exactl

ALT The Diophantine equation FāĖ£+FāŹø=2įµ, where Fā denotes the k-th Fibonacci number and n,m,aā ā¤ā„ā, has attracted attention in recent years. The cases (x,y)=(1,1) and (x,y)=(2,2) were completely resolved by Bravo and Luca, and by Jeong and Park, respectively. In this note, we investigate the mixed exponent case (x,y)=(2,1) and we completely determine all nonnegative integer solutions.

ALT We study a family of special numbers and polynomials introduced by Simsek whose exponential generating function has as denominator a falling factorial in the exponential variable. Using the partial fraction decomposition of this denominator, each member of the family is expressed by a single finite sum involving Bernoulli polynomials, Apostol Bernoulli polynomials and two variable Fubini polynomials evaluated at reciprocals of integers. A second expansion, around the point where the denominator vanishes, expresses the same numbers through Stirling numbers of the second kind and generalized harmonic numbers, and yields closed formulas for the first few members. We construct a function, built from the Hurwitz zeta function and Lerch s transcendent, which interpolates the polynomials at the negative integers and gives a closed form of a multiple series recently introduced by Pokaz, Ribicic Penava and Simsek, we give an Euler type integral representation for it, and show that the numbers a

