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Normalized Ricci flow on Riemann surfaces and determinants of Laplacian 9 0 0 A. Kokotov∗and D. Korotkin † 2 n January 12, 2009 a J 0 1 Department of Mathematics and Statistics, Concordia University ] P 7141 Sherbrook West, Montreal H4B 1R6, Quebec, Canada S . h t a m [ 2 Abstract. In this note wegive asimpleproof of thefact that the determinantof Laplace operator v in smooth metric over compact Riemann surfaces of arbitrary genus g monotonously grows under the 0 1 normalized Ricciflow. Together withresultsofHamilton thatundertheaction ofthenormalizedRicci 0 flow the smooth metric tends asymptotically to metric of constant curvature for g ≥ 1, this leads to a 5 simple proof of Osgood-Phillips-Sarnak theorem stating that within the class of smooth metrics with 0 4 fixed conformal class and fixed volume the determinant of Laplace operator is maximal on metric of 0 constant curvatute. / h t a m The normalized Ricci flow on compact Riemann surface of arbitrary genus g was introduced by : Hamilton [1]. Under the action of the normalized Ricci flow the smooth metric g evolves according v ij i to the following differential equation: X r ∂ a gij = (R0−R)gij (0.1) ∂t where R is the scalar curvature, and R0 is its average value. It was proved in [1] that solution of equation (0.1) exists for all times and that asymptotically, as t → ∞, the metric converges to the metric of constant curvature for R0 ≤ 0, i.e. both for g = 1 (when R0 = 0) and g ≥2 (when R0 < 0). For g = 0 the sufficient condition of convergency of the metric to metric of constant curvature is the global condition R > 0 for t = 0. The volume of the Riemann surface remains constant under the action of normalized Ricci flow (0.1). In this note we give a simple proof to the following theorem (although this statement in principle follows from results of [4], the proof given here seems essentailly simpler): ∗e-mail: [email protected] †e-mail: [email protected] 1 Theorem 1 The determinant of Laplace operator in smooth metric over compact Riemann surface L monotonously increases under the action of Ricci flow (0.1). Proof. Write the metric in the diagonal form g = ρ(z,z¯)δ ; then the normalized Ricci flow takes ij ij the form ∂ logρ = R0−R (0.2) ∂t where 1 R = − (logρ)zz¯ , (0.3) ρ Rdµ R0 = L (0.4) µ R L where µ = ρdz ∧dz¯. Consider Alvarez-Polyakov forRmula [2, 3] for variation of det∆ with respect to an arbitrary one-parametric infinitesimal variation of the metric in fixed conformal class: ∂ logdet∆ 1 = (logρ) (−ρR)dz∧dz¯ (0.5) ∂t detℑB 12π t (cid:26) (cid:27) ZL which for the Ricci flow (0.2) equals 2 −1 −1 (R0−R)Rdµ = Rdµ − dµ R2dµ ≥ 0 (0.6) 12 12 dµ ZL L ((cid:18)ZL (cid:19) ZL ZL ) according to Cauchy inequality ( fgdµ)2R≤( f2)( g2) for f = 1, g = R. L L L Since the matrix of b-periods does not change under the Ricci flow, we get R R R ∂ logdet∆ ≥ 0 ; (0.7) ∂t the equality takes place only if R = const i.e. only for the metrics of constant curvature, which are stationary points of Ricci flow. The following corollary reproduces one of the results of the paper [4]: Corollary 1 On the space of smooth metrics on Riemann surfaces of volume 1 and genus g ≥ 1 with fixed conformal structure the determinant has maximum on the metric of constant curvature (0 for g = 1 and −1 for d≥ 2). Proof follows from from Th.1 if we take into account results of Hamilton [1] that in g ≥ 1 asymp- totically, as t → ∞,any smoothmetrictendsunderthenormalized Ricciflowtothemetricofconstant curvature (of the same volume). For genus zero resultsof [1]implya weaker version of Colollary 1, whichstates that thedeterminat of Laplacian achieves its maximum on the metric of constant curvature within the class of smooth metrics with fixed volume whose curvature is everywhere positive. We know a few recent results similar to Th.1. In [5] it was proved that the determinant of Laplace operator monotonously increases under Calabi flow [5]. In [6] it was proved that the first eigenvalue of Laplacian always increases under the action of (non-normalized) Ricci flow; however, since the 2 non-normalized Ricci flow does not preserve the volume, the does not lead to a statement similar to Corollary 1 for the first eigenvalue. Remark (added December 2008). Recently Werner Mu¨ller informed us that the theorem proved in this note was proved in Section 3 of the earlier paper ([7]. References [1] R.S.Hamilton, The Ricci flow on surfaces, Contemporary Math. 71 237-262 (1988) [2] O.Alvarez, Theory of strings with boundaries, Nucl.Phys. B216 125-184 (1983) [3] Polyakov, Quantum geometry of bosonic strings, Phys.Lett. 103B, 211-213 (1981) [4] B.Osgood, R.Phillips, P.Sarnak, Extremals of determinants of Laplacians. J. Funct. Anal. 80 148-211 (1988) [5] X.X.Chen,CalabiflowonRiemannsurfacesrevisited: anewpointofview,IMRN,2001:6275-297 (2001) [6] Li Ma, Eigen-value monotonicity for the Ricci-Hamilton flow, math.DG/0403065 [7] W.Mu¨ller, K.Wendland, Extremal Ka¨hler metrics and Ray-Singer analytic torsion, Geometric aspects of partial differential equations (Roskilde, 1998), 135-160, Contemp.math., 242 AMS, Providence, RI (1999), arXiv:math/9904048 3

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