- The paper identifies conditions under which solutions to the Diophantine equation with consecutive exponents are either a unique solution or constrained to specific values.
- One case the paper examines involves factorization of $2p+1$ into coprime, consecutive odd primes; methods used include modular reduction and valuations via the Lifting-the-Exponent Lemma.
- The above factorization is iteratively scaled to fit through logarithmic bound constraints and the equation $ p^x+(2p+1)^y = z^2 $ (scaling factor $(2k^2-1)^{b+1})$.
The paper studies the exponential Diophantine equation
px+(2p+1)y=z2
over positive integers x, y, z, where p is an odd prime and the exponents are required to be consecutive, i.e., ∣x−y∣=1 (2608.18608). The novelty relative to earlier work on equations of the form ax+by=z2 is twofold: the pair (p,2p+1) is treated uniformly without assuming that $2p+1$ is prime, and the consecutive-exponent condition—previously examined only for specific pairs such as (43,87) by Gaha and Mezroui—is handled for the entire one-parameter family.
Main result
The central theorem establishes a dichotomy. For every odd prime x0, exactly one of the following holds:
- Case (i): the unique solution in positive integers is
x1
which follows from the identity x2.
- Case (ii): any exceptional solution can occur only when x3 is composite and factors into coprime consecutive odd integers,
x4
with the exponents tied to a parameter satisfying
x5
The logarithmic bound reduces the problem to finitely many candidate exponents for each fixed prime, converting an infinite family into a decidable finite check per value of x6. A concrete exceptional solution exists at x7: for x8 one has x9, i.e., y0.
Method of proof
The argument is elementary throughout, relying on coprimality factorizations, modular order arguments, and the Lifting-the-Exponent (LTE) lemma (2608.18608). Since y1 and y2 are consecutive, they have opposite parity, which splits the problem cleanly.
Case A (y3 odd, y4 even). Writing y5, y6 yields y7 with y8. The two factors are shown to be coprime, so their product being a prime power forces y9, giving z0. Both parity-consistent sub-cases (z1 and z2) are then eliminated by reduction modulo z3: the congruence forces z4, hence z5; reduction modulo z6 then requires z7 via z8, contradicting oddness of z9. This case therefore admits no solutions with p0. The boundary case p1 produces only p2, which is outside the stated domain since p3 must be positive—a small assumption worth noting when comparing with literature that permits p4.
Case B (p5 even, p6 odd). Writing p7, p8 gives p9.
- Trivial split (∣x−y∣=10): this yields ∣x−y∣=11. For the sub-case ∣x−y∣=12, LTE gives ∣x−y∣=13, so any solution requires ∣x−y∣=14, hence ∣x−y∣=15; an induction shows ∣x−y∣=16 for all ∣x−y∣=17, while ∣x−y∣=18 fails by direct computation. This isolates the unique solution ∣x−y∣=19, namely ax+by=z20. The sub-case ax+by=z21 fails by a simple size comparison, ax+by=z22.
- Non-trivial split: both factors exceed ax+by=z23, so coprimality forces ax+by=z24 with ax+by=z25, ax+by=z26, and ax+by=z27. A gcd argument shows ax+by=z28 where ax+by=z29, so (p,2p+1)0; (p,2p+1)1 contradicts integrality of (p,2p+1)2, leaving (p,2p+1)3, i.e., (p,2p+1)4, (p,2p+1)5, and (p,2p+1)6 prime. Within this structure, the sub-case (p,2p+1)7 dies because (p,2p+1)8, so only (p,2p+1)9 survives, yielding the auxiliary equation above.
The logarithmic bound
The finiteness statement follows from pairing terms in the sum and applying AM–GM:
$2p+1$0
while equation (the auxiliary relation rewritten) requires the same sum to equal $2p+1$1. Dividing through gives
$2p+1$2
since $2p+1$3. Taking logarithms yields $2p+1$4, which is the advertised finite range. Note the bound depends on the primality requirement $2p+1$5 being prime; for composite values of $2p+1$6 the factorization argument does not directly apply.
Limitations and open questions
The paper is explicit about what remains unresolved. Computation for $2p+1$7 shows that no further solutions exist among odd $2p+1$8, suggesting $2p+1$9 may be the sole exception to case (i); however, no proof covering all such cases is given, and the author states plainly that determining whether the auxiliary equation admits solutions beyond (43,87)0 is open. Additionally, the dichotomy is conditional on the coprime-factorization hypothesis in case (ii): if (43,87)1 has a square factor or more than two prime factors arranged differently, the reduction to (43,87)2 would require separate treatment, though the gcd analysis of (43,87)3 and (43,87)4 constrains the possibilities considerably. The exclusion of (43,87)5 also leaves the boundary solution (43,87)6 outside the theorem's scope.
Conclusion
This paper resolves the consecutive-exponent Diophantine equation (43,87)7 up to a single finite auxiliary problem: either the unique explicit solution (43,87)8 holds, or (43,87)9 must be a product of twin-odd factors around x00, with exponents confined to x01. The techniques are elementary but carefully deployed—LTE valuations, modular order obstructions, and AM–GM size bounds—and the residual question of uniqueness beyond the example x02 provides a precise target for subsequent work.