arXiv:2207.13155v2
Abstract
Let , where is a Lie group and is a lattice in , let be an open subset of , and let be a one-parameter subsemigroup of . Consider the set of points in whose -orbit misses ; it has measure zero if the flow is ergodic. It has been conjectured that this set has Hausdorff dimension strictly smaller than the dimension of . This conjecture is proved when is compact or when is a simple Lie group of real rank , or, most recently, for certain special flows on the space of lattices. In this paper we prove this conjecture for arbitrary -diagonalizable flows on irreducible quotients of semisimple Lie groups. The proof uses exponential mixing of the flow together with the method of integral inequalities for height functions on . We also derive an application to jointly Dirichlet-Improvable systems of linear forms.
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Detailed mathematical audit
01Statements4 reported findingsCorrect
The abstract dimension-drop theorem under effective equidistribution and effective nondivergence, its semisimple homogeneous-space corollary, and the jointly Dirichlet-improvable dimension bound are correct. The matrix-space symbols in the last application have a unique harmless correction.
EEP and ENDP imply uniform leafwise dimension drop
Pages 4–7 and 26–29 · Theorems 1.5, 2.1, and Section 9 · arXiv:2207.13155v2
EEP supplies a uniform covering loss for orbit segments remaining in a suitable compact set, while ENDP supplies an independent covering loss for segments making repeated cusp excursions. Proposition 8.1 combines the two alternatives over blocks, and Theorem 2.1 converts the resulting covering number into positive Hausdorff codimension. The final choices of the compact set, scale, block length, and Margulis constant make the lower bound positive uniformly in the base point.
Dimension drop on the full homogeneous space
Pages 5 and 7–8 · Corollary 1.6 and its proof · arXiv:2207.13155v2
For the semisimple products in Theorem 1.4, the expanding horospherical subgroup has ENDP from the cited height-function construction and EEP from exponential mixing. The local product of expanding and nonexpanding directions lets the leafwise bound of Theorem 1.5 be sliced with the complementary factor, giving dimension strictly below for the global exceptional set.
Joint Dirichlet improvement has dimension drop
Pages 30–31 · Theorem 10.1 and Equations (10.3)–(10.5) · arXiv:2207.13155v2
The lattice correspondence turns joint -improvement into eventual avoidance of by the product diagonal flow. The product expanding horospherical subgroup has ENDP componentwise and EEP because exponential mixing tensorizes over finitely many factors. Theorem 1.5 therefore gives positive codimension in the -dimensional matrix parameter space.
The matrix dimensions are transposed
Page 31 · definition of jointly -Dirichlet-improvable tuples and Equation (10.4) · arXiv:2207.13155v2
The text places in , but with and requires . Replace both displayed occurrences of by . Also replace the mixed delimiter in (10.4) by . The earlier definition, the matrices , and the dimension make these corrections unique.
02Proofs6 reported findingsCorrect
The EEP covering, Margulis-inequality iteration, combined block argument, and product-flow application are correct and complete. Four literal normalization, rate-notation, target-letter, and property-name errors, together with one local inner-core scale correction, have unique repairs and do not change the arguments.
Compact and cuspidal covering estimates combine correctly
Pages 11–29 · Propositions 4.4, 6.1, 8.1, and proof of Theorem 2.1 · arXiv:2207.13155v2
The smoothed indicator estimate from EEP bounds the number of compact-part Bowen boxes. Iterating the Margulis inequality controls the height integral over cusp blocks, and Markov's inequality gives the ENDP covering count. Proposition 8.1 partitions itineraries by the two block types and keeps the overlap factors explicit. The parameter choices in Section 9 make the combined exponential base smaller than the full Bowen growth rate, which yields the claimed codimension.
The normalized ball radius should be one
Page 2 · notation paragraph before Definition 1.1 · arXiv:2207.13155v2
The paper says that Haar measure is normalized so that , which cannot hold for every variable radius . Replace by . Section 6 explicitly uses , confirming the unique intended normalization.
The Bowen exponents are written as eigenvalues of
Pages 5–6 and 9 · Equations (2.3), (2.4), and the definition of · arXiv:2207.13155v2
The element belongs to the group, so is not the infinitesimal adjoint map whose positive eigenvalues produce the factors and the Haar scaling . Let and use in these definitions; equivalently, take logarithms of the eigenvalues of . All following conjugation and measure formulas already use these infinitesimal rates, making the repair unique and harmless.
The inner-core scale must be chosen below the defining supremum
Pages 6–7 · definition of and Equation (2.14) in the proof of Theorem 1.5 · arXiv:2207.13155v2
Equation (2.14) must read , not , because the next step subtracts two error terms from this quantity. In addition, the printed choice can attain the supremum in the definition of , while the definition alone guarantees the measure inequality only strictly below that supremum. Replace it by . Since the later radius satisfies , one still has ; all subsequent parameter conditions and the codimension bound are unchanged. This local choice and the sign correction give the required lower bound without assuming an unstated continuity property.
The target set changes from to an undefined
Page 8 · paragraph before the Wegmann product estimate · arXiv:2207.13155v2
After fixing the open set , the proof says that belongs to . Replace by . The preceding distance estimate and every set in the following dimension calculation use .
Exponential mixing supplies EEP, not a second copy of ENDP
Page 31 · paragraph immediately before Theorem 10.1 · arXiv:2207.13155v2
Theorem 1.4 first supplies ENDP for . The next sentence invokes exponential mixing and Theorem 1.2 but again says that has ENDP. Replace the second ENDP by EEP. With both distinct properties available, the stated application of Theorem 1.5 follows.
03Novelty0 reported findingsNo non-novelty findings
No non-novelty findings.