skip to main content
US FlagAn official website of the United States government
dot gov icon
Official websites use .gov
A .gov website belongs to an official government organization in the United States.
https lock icon
Secure .gov websites use HTTPS
A lock ( lock ) or https:// means you've safely connected to the .gov website. Share sensitive information only on official, secure websites.


Title: Smooth rigidity for codimension one Anosov flows
We introduce the matching functions technique in the setting of Anosov flows. Then we observe that simple periodic cycle functionals (also known as temporal distances) provide a source of matching functions for conjugate Anosov flows. For conservative codimension one Anosov flows φ<#comment/> t :<#comment/> M →<#comment/> M \varphi ^t\colon M\to M , dim ⁡<#comment/> M ≥<#comment/> 4 \dim M\ge 4 , these simple periodic cycle functionals are C 1 C^1 regular and, hence, can be used to improve regularity of the conjugacy. Specifically, we prove that a continuous conjugacy must, in fact, be a C 1 C^1 diffeomorphism for an open and dense set of codimension one conservative Anosov flows.  more » « less
Award ID(s):
1955564 1900778
PAR ID:
10468056
Author(s) / Creator(s):
;
Publisher / Repository:
AMS
Date Published:
Journal Name:
Proceedings of the American Mathematical Society
Volume:
151
Issue:
769
ISSN:
0002-9939
Page Range / eLocation ID:
2975 to 2988
Format(s):
Medium: X
Sponsoring Org:
National Science Foundation
More Like this
  1. Let Ω<#comment/> + ⊂<#comment/> R n + 1 \Omega ^+\subset \mathbb {R}^{n+1} be a bounded δ<#comment/> \delta -Reifenberg flat domain, with δ<#comment/> > 0 \delta >0 small enough, possibly with locally infinite surface measure. Assume also that Ω<#comment/> −<#comment/> = R n + 1 ∖<#comment/> Ω<#comment/> + ¯<#comment/> \Omega ^-= \mathbb {R}^{n+1}\setminus \overline {\Omega ^+} is an NTA (non-tangentially accessible) domain as well and denote by ω<#comment/> + \omega ^+ and ω<#comment/> −<#comment/> \omega ^- the respective harmonic measures of Ω<#comment/> + \Omega ^+ and Ω<#comment/> −<#comment/> \Omega ^- with poles p ±<#comment/> ∈<#comment/> Ω<#comment/> ±<#comment/> p^\pm \in \Omega ^\pm . In this paper we show that the condition that log ⁡<#comment/> d ω<#comment/> −<#comment/> d ω<#comment/> + ∈<#comment/> VMO ⁡<#comment/> ( ω<#comment/> + ) \log \dfrac {d\omega ^-}{d\omega ^+} \in \operatorname {VMO}(\omega ^+) is equivalent to Ω<#comment/> + \Omega ^+ being a chord-arc domain with inner unit normal belonging to VMO ⁡<#comment/> ( H n | ∂<#comment/> Ω<#comment/> + ) \operatorname {VMO}(\mathcal {H}^n|_{\partial \Omega ^+})
    more » « less
  2. In this paper we derive the best constant for the following L ∞<#comment/> L^{\infty } -type Gagliardo-Nirenberg interpolation inequality ‖<#comment/> u ‖<#comment/> L ∞<#comment/> ≤<#comment/> C q , ∞<#comment/> , p ‖<#comment/> u ‖<#comment/> L q + 1 1 −<#comment/> θ<#comment/> ‖<#comment/> ∇<#comment/> u ‖<#comment/> L p θ<#comment/> , θ<#comment/> = p d d p + ( p −<#comment/> d ) ( q + 1 ) , \begin{equation*} \|u\|_{L^{\infty }}\leq C_{q,\infty ,p} \|u\|^{1-\theta }_{L^{q+1}}\|\nabla u\|^{\theta }_{L^p},\quad \theta =\frac {pd}{dp+(p-d)(q+1)}, \end{equation*} where parameters q q and p p satisfy the conditions p > d ≥<#comment/> 1 p>d\geq 1 , q ≥<#comment/> 0 q\geq 0 . The best constant C q , ∞<#comment/> , p C_{q,\infty ,p} is given by C q , ∞<#comment/> , p = θ<#comment/> −<#comment/> θ<#comment/> p ( 1 −<#comment/> θ<#comment/> ) θ<#comment/> p M c −<#comment/> θ<#comment/> d , M c ∫<#comment/> R d u c , ∞<#comment/> q + 1 d x , \begin{equation*} C_{q,\infty ,p}=\theta ^{-\frac {\theta }{p}}(1-\theta )^{\frac {\theta }{p}}M_c^{-\frac {\theta }{d}},\quad M_c≔\int _{\mathbb {R}^d}u_{c,\infty }^{q+1} dx, \end{equation*} where u c , ∞<#comment/> u_{c,\infty } is the unique radial non-increasing solution to a generalized Lane-Emden equation. The case of equality holds when u = A u c , ∞<#comment/> ( λ<#comment/> ( x −<#comment/> x 0 ) ) u=Au_{c,\infty }(\lambda (x-x_0)) for any real numbers A A , λ<#comment/> > 0 \lambda >0 and x 0 ∈<#comment/> R d x_{0}\in \mathbb {R}^d . In fact, the generalized Lane-Emden equation in R d \mathbb {R}^d contains a delta function as a source and it is a Thomas-Fermi type equation. For q = 0 q=0 or d = 1 d=1 , u c , ∞<#comment/> u_{c,\infty } have closed form solutions expressed in terms of the incomplete Beta functions. Moreover, we show that u c , m →<#comment/> u c , ∞<#comment/> u_{c,m}\to u_{c,\infty } and C q , m , p →<#comment/> C q , ∞<#comment/> , p C_{q,m,p}\to C_{q,\infty ,p} as m →<#comment/> + ∞<#comment/> m\to +\infty for d = 1 d=1 , where u c , m u_{c,m} and C q , m , p C_{q,m,p} are the function achieving equality and the best constant of L m L^m -type Gagliardo-Nirenberg interpolation inequality, respectively. 
    more » « less
  3. Let f f be analytic on [ 0 , 1 ] [0,1] with | f ( k ) ( 1 / 2 ) | ⩽<#comment/> A α<#comment/> k k ! |f^{(k)}(1/2)|\leqslant A\alpha ^kk! for some constants A A and α<#comment/> > 2 \alpha >2 and all k ⩾<#comment/> 1 k\geqslant 1 . We show that the median estimate of μ<#comment/> = ∫<#comment/> 0 1 f ( x ) d x \mu =\int _0^1f(x)\,\mathrm {d} x under random linear scrambling with n = 2 m n=2^m points converges at the rate O ( n −<#comment/> c log ⁡<#comment/> ( n ) ) O(n^{-c\log (n)}) for any c > 3 log ⁡<#comment/> ( 2 ) / π<#comment/> 2 ≈<#comment/> 0.21 c> 3\log (2)/\pi ^2\approx 0.21 . We also get a super-polynomial convergence rate for the sample median of 2 k −<#comment/> 1 2k-1 random linearly scrambled estimates, when k / m k/m is bounded away from zero. When f f has a p p ’th derivative that satisfies a λ<#comment/> \lambda -Hölder condition then the median of means has error O ( n −<#comment/> ( p + λ<#comment/> ) + ϵ<#comment/> ) O( n^{-(p+\lambda )+\epsilon }) for any ϵ<#comment/> > 0 \epsilon >0 , if k →<#comment/> ∞<#comment/> k\to \infty as m →<#comment/> ∞<#comment/> m\to \infty . The proof techniques use methods from analytic combinatorics that have not previously been applied to quasi-Monte Carlo methods, most notably an asymptotic expression from Hardy and Ramanujan on the number of partitions of a natural number. 
    more » « less
  4. We prove that for any countable directed graph E E with Condition (K), the associated graph C ∗<#comment/> C^* -algebra C ∗<#comment/> ( E ) C^*(E) has nuclear dimension at most 2 2 . Furthermore, we provide a sufficient condition producing an upper bound of 1 1
    more » « less
  5. We formulate and prove a Conner–Floyd isomorphism for the algebraic K-theory of arbitrary qcqs derived schemes. To that end, we study a stable ∞<#comment/> \infty -category of non- A 1 \mathbb {A}^1 -invariant motivic spectra, which turns out to be equivalent to the ∞<#comment/> \infty -category of fundamental motivic spectra satisfying elementary blowup excision, previously introduced by the first and third authors. We prove that this ∞<#comment/> \infty -category satisfies P 1 \mathbb {P}^1 -homotopy invariance and weighted A 1 \mathbb {A}^1 -homotopy invariance, which we use in place of A 1 \mathbb {A}^1 -homotopy invariance to obtain analogues of several key results from A 1 \mathbb {A}^1 -homotopy theory. These allow us in particular to define a universal oriented motivic E ∞<#comment/> \mathbb {E}_\infty -ring spectrum M G L \mathrm {MGL} . We then prove that the algebraic K-theory of a qcqs derived scheme X X can be recovered from its M G L \mathrm {MGL} -cohomology via a Conner–Floyd isomorphism\[ M G L ∗<#comment/> ∗<#comment/> ( X ) ⊗<#comment/> L Z [ β<#comment/> ±<#comment/> 1 ] ≃<#comment/> K ∗<#comment/> ∗<#comment/> ( X ) , \mathrm {MGL}^{**}(X)\otimes _{\mathrm {L}{}}\mathbb {Z}[\beta ^{\pm 1}]\simeq \mathrm {K}{}^{**}(X), \]where L \mathrm {L}{} is the Lazard ring and K p , q ( X ) = K 2 q −<#comment/> p ( X ) \mathrm {K}{}^{p,q}(X)=\mathrm {K}{}_{2q-p}(X) . Finally, we prove a Snaith theorem for the periodized version of M G L \mathrm {MGL}
    more » « less