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: The $$L^p$$-Fisher–Rao metric and Amari–C̆encov $$\alpha $$-Connections
Abstract We introduce a family of Finsler metrics, called the$$L^p$$ L p -Fisher–Rao metrics$$F_p$$ F p , for$$p\in (1,\infty )$$ p ( 1 , ) , which generalizes the classical Fisher–Rao metric$$F_2$$ F 2 , both on the space of densities$${\text {Dens}}_+(M)$$ Dens + ( M ) and probability densities$${\text {Prob}}(M)$$ Prob ( M ) . We then study their relations to the Amari–C̆encov$$\alpha $$ α -connections$$\nabla ^{(\alpha )}$$ ( α ) from information geometry: on$${\text {Dens}}_+(M)$$ Dens + ( M ) , the geodesic equations of$$F_p$$ F p and$$\nabla ^{(\alpha )}$$ ( α ) coincide, for$$p = 2/(1-\alpha )$$ p = 2 / ( 1 - α ) . Both are pullbacks of canonical constructions on$$L^p(M)$$ L p ( M ) , in which geodesics are simply straight lines. In particular, this gives a new variational interpretation of$$\alpha $$ α -geodesics as being energy minimizing curves. On$${\text {Prob}}(M)$$ Prob ( M ) , the$$F_p$$ F p and$$\nabla ^{(\alpha )}$$ ( α ) geodesics can still be thought as pullbacks of natural operations on the unit sphere in$$L^p(M)$$ L p ( M ) , but in this case they no longer coincide unless$$p=2$$ p = 2 . Using this transformation, we solve the geodesic equation of the$$\alpha $$ α -connection by showing that the geodesic are pullbacks of projections of straight lines onto the unit sphere, and they always cease to exists after finite time when they leave the positive part of the sphere. This unveils the geometric structure of solutions to the generalized Proudman–Johnson equations, and generalizes them to higher dimensions. In addition, we calculate the associate tensors of$$F_p$$ F p , and study their relation to$$\nabla ^{(\alpha )}$$ ( α ) more » « less
Award ID(s):
1953244
PAR ID:
10490304
Author(s) / Creator(s):
; ; ;
Publisher / Repository:
Springer Science + Business Media
Date Published:
Journal Name:
Calculus of Variations and Partial Differential Equations
Volume:
63
Issue:
2
ISSN:
0944-2669
Format(s):
Medium: X
Sponsoring Org:
National Science Foundation
More Like this
  1. Abstract A measurement of the dijet production cross section is reported based on proton–proton collision data collected in 2016 at$$\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V} $$ s = 13 Te V by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3$$\,\text {fb}^{-1}$$ fb - 1 . Jets are reconstructed with the anti-$$k_{\textrm{T}} $$ k T algorithm for distance parameters of$$R=0.4$$ R = 0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity$$|y |_{\text {max}} $$ | y | max of the two jets with the highest transverse momenta$$p_{\textrm{T}}$$ p T and their invariant mass$$m_{1,2} $$ m 1 , 2 , and triple-differentially (3D) as a function of the rapidity separation$$y^{*} $$ y , the total boost$$y_{\text {b}} $$ y b , and either$$m_{1,2} $$ m 1 , 2 or the average$$p_{\textrm{T}}$$ p T of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the$${\text {Z}} $$ Z boson is investigated, yielding a value of$$\alpha _\textrm{S} (m_{{\text {Z}}}) =0.1179\pm 0.0019$$ α S ( m Z ) = 0.1179 ± 0.0019
    more » « less
  2. Abstract A measurement is presented of a ratio observable that provides a measure of the azimuthal correlations among jets with large transverse momentum$$p_{\textrm{T}}$$ p T . This observable is measured in multijet events over the range of$$p_{\textrm{T}} = 360$$ p T = 360 –$$3170\,\text {Ge}\hspace{-.08em}\text {V} $$ 3170 Ge V based on data collected by the CMS experiment in proton-proton collisions at a centre-of-mass energy of 13$$\,\text {Te}\hspace{-.08em}\text {V}$$ Te V , corresponding to an integrated luminosity of 134$$\,\text {fb}^{-1}$$ fb - 1 . The results are compared with predictions from Monte Carlo parton-shower event generator simulations, as well as with fixed-order perturbative quantum chromodynamics (pQCD) predictions at next-to-leading-order (NLO) accuracy obtained with different parton distribution functions (PDFs) and corrected for nonperturbative and electroweak effects. Data and theory agree within uncertainties. From the comparison of the measured observable with the pQCD prediction obtained with the NNPDF3.1 NLO PDFs, the strong coupling at the Z boson mass scale is$$\alpha _\textrm{S} (m_{{\textrm{Z}}}) =0.1177 \pm 0.0013\, \text {(exp)} _{-0.0073}^{+0.0116} \,\text {(theo)} = 0.1177_{-0.0074}^{+0.0117}$$ α S ( m Z ) = 0.1177 ± 0.0013 (exp) - 0.0073 + 0.0116 (theo) = 0 . 1177 - 0.0074 + 0.0117 , where the total uncertainty is dominated by the scale dependence of the fixed-order predictions. A test of the running of$$\alpha _\textrm{S}$$ α S in the$$\,\text {Te}\hspace{-.08em}\text {V}$$ Te V region shows no deviation from the expected NLO pQCD behaviour. 
    more » « less
  3. Abstract Schinzel and Wójcik have shown that for every$$\alpha ,\beta \in \mathbb {Q}^{\times }\hspace{0.55542pt}{\setminus }\hspace{1.111pt}\{\pm 1\}$$ α , β Q × \ { ± 1 } , there are infinitely many primespwhere$$v_p(\alpha )=v_p(\beta )=0$$ v p ( α ) = v p ( β ) = 0 and where$$\alpha $$ α and$$\beta $$ β generate the same multiplicative group modp. We prove a weaker result in the same direction for algebraic numbers$$\alpha , \beta $$ α , β . Let$$\alpha , \beta \in \overline{\mathbb {Q}} ^{\times }$$ α , β Q ¯ × , and suppose$$|N_{\mathbb {Q}(\alpha ,\beta )/\mathbb {Q}}(\alpha )|\ne 1$$ | N Q ( α , β ) / Q ( α ) | 1 and$$|N_{\mathbb {Q}(\alpha ,\beta )/\mathbb {Q}}(\beta )|\ne 1$$ | N Q ( α , β ) / Q ( β ) | 1 . Then for some positive integer$$C = C(\alpha ,\beta )$$ C = C ( α , β ) , there are infinitely many prime idealsPof Equation missing<#comment/>where$$v_P(\alpha )=v_P(\beta )=0$$ v P ( α ) = v P ( β ) = 0 and where the group$$\langle \beta \bmod {P}\rangle $$ β mod P is a subgroup of$$\langle \alpha \bmod {P}\rangle $$ α mod P with$$[\langle \alpha \bmod {P}\rangle \,{:}\, \langle \beta \bmod {P}\rangle ]$$ [ α mod P : β mod P ] dividingC. A key component of the proof is a theorem of Corvaja and Zannier bounding the greatest common divisor of shiftedS-units. 
    more » « less
  4. Abstract The elliptic flow$$(v_2)$$ ( v 2 ) of$${\textrm{D}}^{0}$$ D 0 mesons from beauty-hadron decays (non-prompt$${\textrm{D}}^{0})$$ D 0 ) was measured in midcentral (30–50%) Pb–Pb collisions at a centre-of-mass energy per nucleon pair$$\sqrt{s_{\textrm{NN}}} = 5.02$$ s NN = 5.02  TeV with the ALICE detector at the LHC. The$${\textrm{D}}^{0}$$ D 0 mesons were reconstructed at midrapidity$$(|y|<0.8)$$ ( | y | < 0.8 ) from their hadronic decay$$\mathrm {D^0 \rightarrow K^-\uppi ^+}$$ D 0 K - π + , in the transverse momentum interval$$2< p_{\textrm{T}} < 12$$ 2 < p T < 12  GeV/c. The result indicates a positive$$v_2$$ v 2 for non-prompt$${{\textrm{D}}^{0}}$$ D 0 mesons with a significance of 2.7$$\sigma $$ σ . The non-prompt$${{\textrm{D}}^{0}}$$ D 0 -meson$$v_2$$ v 2 is lower than that of prompt non-strange D mesons with 3.2$$\sigma $$ σ significance in$$2< p_\textrm{T} < 8~\textrm{GeV}/c$$ 2 < p T < 8 GeV / c , and compatible with the$$v_2$$ v 2 of beauty-decay electrons. Theoretical calculations of beauty-quark transport in a hydrodynamically expanding medium describe the measurement within uncertainties. 
    more » « less
  5. Abstract It has been recently established in David and Mayboroda (Approximation of green functions and domains with uniformly rectifiable boundaries of all dimensions.arXiv:2010.09793) that on uniformly rectifiable sets the Green function is almost affine in the weak sense, and moreover, in some scenarios such Green function estimates are equivalent to the uniform rectifiability of a set. The present paper tackles a strong analogue of these results, starting with the “flagship degenerate operators on sets with lower dimensional boundaries. We consider the elliptic operators$$L_{\beta ,\gamma } =- {\text {div}}D^{d+1+\gamma -n} \nabla $$ L β , γ = - div D d + 1 + γ - n associated to a domain$$\Omega \subset {\mathbb {R}}^n$$ Ω R n with a uniformly rectifiable boundary$$\Gamma $$ Γ of dimension$$d < n-1$$ d < n - 1 , the now usual distance to the boundary$$D = D_\beta $$ D = D β given by$$D_\beta (X)^{-\beta } = \int _{\Gamma } |X-y|^{-d-\beta } d\sigma (y)$$ D β ( X ) - β = Γ | X - y | - d - β d σ ( y ) for$$X \in \Omega $$ X Ω , where$$\beta >0$$ β > 0 and$$\gamma \in (-1,1)$$ γ ( - 1 , 1 ) . In this paper we show that the Green functionGfor$$L_{\beta ,\gamma }$$ L β , γ , with pole at infinity, is well approximated by multiples of$$D^{1-\gamma }$$ D 1 - γ , in the sense that the function$$\big | D\nabla \big (\ln \big ( \frac{G}{D^{1-\gamma }} \big )\big )\big |^2$$ | D ( ln ( G D 1 - γ ) ) | 2 satisfies a Carleson measure estimate on$$\Omega $$ Ω . We underline that the strong and the weak results are different in nature and, of course, at the level of the proofs: the latter extensively used compactness arguments, while the present paper relies on some intricate integration by parts and the properties of the “magical distance function from David et al. (Duke Math J, to appear). 
    more » « less