diff --git "a/data_all_eng_slimpj/shuffled/split2/finalzzjehv" "b/data_all_eng_slimpj/shuffled/split2/finalzzjehv" new file mode 100644--- /dev/null +++ "b/data_all_eng_slimpj/shuffled/split2/finalzzjehv" @@ -0,0 +1,5 @@ +{"text":"\\section{Introduction and Statement of the Result}\n\nThe curvature of the Weil-Pe\\-ters\\-son\\ metric recently attracted further interest. In this note we will give the precise estimate for the average of the scalar curvature $S_{WP}$ of the Weil-Petersson metric on the moduli space $\\ol{\\mathcal M} _g$ as $g$ tends to infinity. The result is the value\n$$\n \\frac{1}{(g-1)} \\frac{\\bigintss_{\\ol{\\cM}_g} \\, (-S_{W\\! P})\\,dV_{W \\! P}}{\\bigintss_{\\ol{\\cM}_g} dV_{W\\! P}} = \\frac{13}{4\\pi} + \\frac{\\pi}{12} \\frac{1}{g} + \\left( \\frac{1}{4\\pi} +\\frac{\\pi}{12} \\right) \\frac{1}{g^2}+ O\\left(\\frac{1}{g^3}\\right).\n$$\nThe proof of the asymptotics will be based upon methods of Algebraic Geometry. Wolpert showed in \\cite{wo1,wo2} that Mumford's canonical class $\\kappa_1$ (the tautological class obtained from the universal curve) from \\cite{mu1,mu2} (cf.\\ \\cite{ac,ac2}) is the cohomology of the Weil-Pe\\-ters\\-son\\ form extended to the compactification up to the factor $2\\pi^2$ together with the fact that its restriction to the boundary equals to the Weil-Pe\\-ters\\-son\\ cohomomology of the boundary (interpreted as related to moduli of punctured surfaces of lower genus).\n\nThe finiteness of the Weil-Pe\\-ters\\-son\\ volume itself is a consequence of Masur's estimates \\cite{ma}, whereas the curvature was computed by Wolpert \\cite{wo3} and Fischer-Tromba \\cite{tro}. These results implied strong negativity properties, in particular the strict negativity of the scalar curvature. It is known that the scalar curvature tends to $-\\infty $ towards the boundary. Precise estimates of the curvature of the Weil-Pe\\-ters\\-son\\ metric towards the boundary are contained in \\cite{s} \\and \\cite{t} with a later developments by Liu-Sun-Yau \\cite{lsy1,lsy2}.\n\nEstimates of the Weil-Pe\\-ters\\-son\\ volume had been given by Mirzakhani \\cite{mi}, Mirzakhani-Zograf \\cite{m-z}, Penner \\cite{pe}, Grushevsky \\cite{gru}, Zograf \\cite{zo2,zo} and previously in \\cite{s-t}. The algebraic aspect is contained in the push-pull formulas by Arbarello and Cornalba \\cite{ac,ac2}.\n\n\nThe Weil-Pe\\-ters\\-son\\ volume of the moduli spaces $\\ol{\\mathcal M} _{g,n}$ of Riemann surfaces of genus $g$ with $n$ punctures is denoted by\n$$\nV_{g,n}=\\int_{{\\mathcal M}_{g,n}}\\kappa_1^{3g-3+n}.\n$$\nFinally the relationship of intersection numbers and volumes as related to two dimensional gravity ought to pointed out. Pertinent references are \\cite{dij,fp,getz,kon,mz,witt}.\n\n\n\nWe showed the following estimates.\n\\begin{theorem}[\\cite{s-t}]\n\\begin{itemize}\n\\item[(i)]\n Let $g>1$. Then\n\\begin{equation}\\label{eq:upper_est}\nV_{g,0} \\geq \\frac{1}{28} V_{g-1,2} + \\frac{1}{672} V_{g-1,1} +\n\\frac{1}{14} \\sum_{j=2}^{[g\/2]} V_{j,1}V_{g-j,1}\n-\\frac{1}{28} (V_{\\frac{g}{2},1})^2 ,\n\\end{equation}\nwith $V_{\\frac{g}{2},1}=0$, if $g$ is odd.\n\\item[(ii)]\nThere exist constants $0 < c < C$, independent of $n$ such that\n\\begin{equation}\\label{eq:asymp1}\nc^g (2g)! \\leq \\frac{V_{g,n}}{(3g-3+n)!} \\leq C^g (2g)!\n\\end{equation}\nfor all fixed $n\\geq 0$ and large $g$.\n\\end{itemize}\n\\end{theorem}\nConcerning \\eqref{eq:asymp1}, a lower estimate for $n=1$ is due to Penner \\cite[Theorem 6.2.2]{pe}, and the upper estimates for $n \\geq 1$ were first shown by Grushevsky in \\cite[Sec.~7]{gru}.\n\nBounds for the curvature of the Weil-Pe\\-ters\\-son\\ metric were proven by Wu and Wolf in \\cite{ww} and Wu in \\cite{wu1,wu2}. A recent result is the following:\n\\begin{theorem}[{Bridgeman-Wu, \\cite{b-w}}]\\label{th:briwu}\nDenote by $S_{W\\!P}$ the scalar curvature of the Weil-Pe\\-ters\\-son\\ form $\\omega_{WP}$, and by $dV_{W\\!P}$ its volume element. There exist constants $0