arXiv:2007.14664v1 [math.DG] 29 Jul 2020 on where h einbuddb h curve, the by bounded region the xlctepeso o eane em nlgu eut o the [17]. - for [6] results an in Analogous obtain generalisations with to [5] harder term. in it remainder obtained makes were a and for here) expression given one explicit (ins 3-dimensional integration a 5-dimensional a of involves incre approach and an area Such metr the the decreases systole. averaging process by averaging proceed the that 299–305) showing pp. 1965, ([4], Berger by inradius. h elpoetv ln eehsoial h rtrslsi systo [3]. [2 in paper book Gromov’s results his by by first 1983 later in the and provided historically was stimulus were Great plane geometry. projective real the acyShazterm rbblsi variance. probabilistic theorem; Cauchy-Schwarz usssoi nqaiysys inequality systolic Pu’s YTLCIEULT IHRMIDRIN REMAINDER WITH INEQUALITY SYSTOLIC A edfieacoe -iesoa 3-dimensional closed a define We given one the and 1952) ([1], Pu in proof original the both that Note e od n phrases. and words Key 2010 o term remainder a with version strengthened a prove to is goal Our for [1] inequality Pu’s and torus the for inequality systolic Loewner’s RP 2 M L ahmtc ujc Classification. Subject Mathematics ntera rjciepae epoeasrne eso fPu’s of version stronger term. a remainder prove metric a We arbitrary with inequality an plane. of systolic projective an area proved real Pu the the and ago. on century systole a the half relating over inequality Pu M. P. student Loewner’s Abstract. ,aaoost onsnsinequality Bonnesen’s to analogous ), stelnt faJra uv nteplane, the in curve Jordan a of length the is = { ( H ELPOETV PLANE PROJECTIVE REAL THE ,w v, IHI .KT N ALNOWIK TAHL AND KATZ G. MIKHAIL h rtppri ytlcgoer a ulse by published was geometry systolic in paper first The ) ∈ R ytl;goercieult;Reana submersion; Riemannian inequality; geometric Systole; 3 × 1. 2. 2 R ( Introduction g 3 h results The ) : ≤ v · π 1 2 R v area( 1 = stecrurdu and circumradius the is rmr 32;Scnay5A0. 53A30 Secondary 53C23; Primary w , g fra rirr metric arbitrary an (for ) · M L w 2 1 = ⊆ − 4 R v , πA 3 × A · ≥ w R steae of area the is 3 π 0 = ysetting by 2 ( R } ssthe ases r cand ic − sthe is tead r ) lic 2 ], g f , 2 MIKHAILG.KATZANDTAHLNOWIK where v w is the scalar product on R3. We have a diffeomorphism M SO(3, R·), (v,w) (v,w,v w), where v w is the vector product→ 3 7→ × × on R . Given a point (v,w) M, the tangent space T(v,w)M can be identified by differentiating the∈ three defining equations of M along a path through (v,w). Thus T M = (X,Y ) R3 R3 : X v =0,Y w =0, X w + Y v =0 . (v,w) { ∈ × · · · · } We define a Riemannian metric gM on M as follows. Given a point (v,w) M, let n = v w and declare the basis (0, n), (n, 0), (w, v) ∈ × − of T(v,w)M to be orthonormal. This metric is a modification of the metric restricted to M from R3 R3 = R6. Namely, with respect to the Euclidean metric on R6 the above× three vectors are orthogonal and the first two have length 1. However, the third vector has Euclidean length √2, whereas we have defined its length to be 1. Thus if A T M denotes the span of (0, n) and (n, 0), and B T M ⊆is (v,w) ⊆ (v,w) spanned by (w, v), then the metric gM on M is obtained from the Euclidean metric−g on R6 (viewed as a quadratic form) as follows: 1 g = g ⇂ + g ⇂ . (2.1) M A 2 B Each of the natural projections p, q : M S2 given by p(v,w) = v and q(v,w)= w, exhibits M as a circle bundle→ over S2.

Lemma 2.1. The maps p and q on (M,gM ) are Riemannian submer- sions, over the unit sphere S2 R3. ⊆ Proof. For the projection p, given (v,w) M, the vector (0, n) as de- fined above is tangent to the fiber p−1(v).∈ The other two vectors, (n, 0) and (w, v), are thus an orthonormal basis for the subspace of T(v,w)M normal to− the fiber, and are mapped by dp to the orthonormal basis n, w 2 of TvS .  The projection p maps the fiber q−1(w) onto a great circle of S2. This map preserves length since the unit vector (n, 0), tangent to the −1 2 fiber q (w) at (v,w), is mapped by dp to the unit vector n TvS . The same comments apply when the roles of p and q are reversed.∈ In the following proposition, integration takes place respectively over great circles C S2, over the fibers in M, over S2, and over M. The integration⊆ is always with respect to the volume element of the given Riemannian metric. Since p and q are Riemannian submersions by Lemma 2.1, we can use Fubini’s Theorem to integrate over M by integrating first over the fibers of either p or q, and then over S2; cf. [18, Lemma 4]. By the remarks above, if C = p(q−1(w)) and f : S2 R → then −1 f p = f. q (w) ◦ C R R SYSTOLIC INEQUALITY WITH REMAINDER IN PROJECTIVE PLANE 3

Proposition 2.2. Given a continuous function f : S2 R+, we de- fine m R by setting m = min f : C S2 a great circle→ . Then ∈ { C ⊆ } m2 1 R 2 f f 2, π ≤ 4π  ZS2  ≤ ZS2 where equality in the second inequality occurs if and only if f is con- stant. Proof. Using the fact that M is the total space of a pair of Riemannian submersions, we obtain 1 f = f p ZS2 ZS2 2π Zp−1(v) ◦  1 = f p 2π ZM ◦ 1 = f p 2π ZS2  Zq−1(w) ◦  1 m =2m, ≥ 2π ZS2 proving the first inequality. By the Cauchy–Schwarz inequality, we have 2 1 f 4π f 2,  ZS2 ·  ≤ ZS2 proving the second inequality. Here equality occurs if and only if f and 1 are linearly dependent, i.e., if and only if f is constant. 

2 1 2 We define the quantity V by setting V = 2 f 2 f . Then f f S − 4π S Proposition 2.2 can be restated as follows. R R  Corollary 2.3. Let f : S2 R+ be continuous. Then → 2 2 m f Vf 0, ZS2 − π ≥ ≥ and Vf =0 if and only if f is constant. Proof. The proof is obtained from Proposition 2.2 by noting that a b c if and only if c a c b 0. ≤ ≤ − ≥ − ≥ We can assign a probabilistic meaning to Vf as follows. Divide the area measure on S2 by 4π, thus turning it into a probability measure µ. A function f : S2 R+ is then thought of as a random variable with → 1 expectation Eµ(f)= 4π S2 f. Its variance is thus given by R 2 2 2 1 2 1 1 Varµ(f)= Eµ(f ) Eµ(f) = f f = Vf . − 4π Z 2 − 4π Z 2  4π  S S 4 MIKHAILG.KATZANDTAHLNOWIK

The variance of a random variable f is non-negative, and it vanishes if and only if f is constant. This reproves the corresponding properties of Vf established above via the Cauchy–Schwarz inequality. Now let g0 be the metric of constant Gaussian K = 1 2 2 2 on RP . The double covering ρ: S (RP ,g0) is a local isometry. Each projective line C RP2 is the→ image under ρ of a great circle of S2. ⊆ Proposition 2.4. Given a function f : RP2 R+, we define m¯ R by setting m¯ = min f : C RP2 a projective→ line . Then ∈ { C ⊆ } R 2¯m2 1 2 f f 2, π ≤ 2π  ZRP2  ≤ ZRP2 where equality in the second inequality occurs if and only if f is con- stant. Proof. We apply Proposition 2.2 to the composition f ρ. Note that ◦ we have −1 f ρ = 2 f and 2 f ρ = 2 2 f. The condition ρ (C) ◦ C S ◦ RP for f toR be constant holdsR since fRis constant ifR and only if f ρ is constant. ◦ 

2 2 1 2 1 For RP we define V¯ = 2 f 2 f = V ◦ . We obtain f RP − 2π RP 2 f ρ the following restatement ofR Proposition 2.4.R  Corollary 2.5. Let f : RP2 R+ be a continuous function. Then → 2 2 2¯m f V¯f 0, ZRP2 − π ≥ ≥ where V¯f =0 if and only if f is constant. 1 RP2 Relative to the probability measure induced by 2π g0 on , we 1 1 2 ¯ have E(f)= 2π RP f, and therefore Var(f)= 2π Vf , providing a prob- abilistic meaningR for the quantity V¯f , as before. By the uniformization theorem, every metric g on RP2 is of the 2 form g = f g0 where g0 is of constant +1, and 2 + 2 the function f : RP R is continuous. The area of g is 2 f , → RP and the g-length of a projective line C is C f. Let L be the shortestR length of a noncontractible loop. Then LR m¯ wherem ¯ is defined in Proposition 2.4, since a projective line in≤RP2 is a noncontractible RP2 2L2 ¯ loop. Then Corollary 2.5 implies area( ,g) π Vf 0. RP2 2L2 ¯ − ≥ ≥ If area( ,g)= π then Vf = 0, which implies that f is constant, by Corollary 2.5. Conversely, if f is a constant c, then the only 2 2L 2 are the projective lines, and therefore L = cπ. Hence π = 2πc = SYSTOLIC INEQUALITY WITH REMAINDER IN PROJECTIVE PLANE 5 area(RP2). We have thus completed the proof of the following result strengthening Pu’s inequality. Theorem 2.6. Let g be a Riemannian metric on RP2. Let L be the shortest length of a noncontractible loop in (RP2,g). Let f : RP2 R+ 2 → be such that g = f g0 where g0 is of constant Gaussian curvature +1. Then 2L2 area(g) 2π Var(f), − π ≥ where the variance is with respect to the probability measure induced 1 2L2 by 2π g0. Furthermore, equality area(g)= π holds if and only if f is constant.

References [1] Pao Ming Pu, Some inequalities in certain nonorientable Riemannian mani- folds, Pacific J. Math. 2 (1952), 55–71. [2] Mikhael Gromov, Filling Riemannian . J. Differential Geom. 18 (1983), no. 1, 1–147. [3] Mikhael Gromov, Metric structures for Riemannian and non-Riemannian spaces, Based on the 1981 French original with appendices by M. Katz, P. Pansu and S. Semmes, Translated from the French by Sean Michael Bates, Progress in Mathematics, 152, Birkh¨auser Boston, Boston, MA, 1999. [4] Marcel Berger, Lectures on geodesics in , Tata Institute of Fundamental Research Lectures on Mathematics, No. 33 Tata Institute of Fundamental Research, Bombay 1965. [5] Charles Horowitz, Karin Usadi Katz, , Loewner’s torus inequality with isosystolic defect, J. Geom. Anal. 19 (2009), no. 4, 796–808. [6] Ivan Babenko, Florent Balacheff, and Guillaume Bulteau, and simplicial complexity for groups, J. Reine Angew. Math. 757 (2019), 247– 277. [7] Florent Balacheff, A local optimal diastolic inequality on the two-sphere, J. Topol. Anal. 2 (2010), no. 1, 109–121. [8] Viktor Bangert, Christopher Croke, Sergei Ivanov, and Mikhail Katz, Bound- ary case of equality in optimal Loewner-type inequalities, Transactions of the American Mathematical Society 359 (2007) (1), 1–17. [9] Paul Creutz, Rigidity of the Pu inequality and quadratic isoperimetric con- stants of normed spaces, preprint (2020). See https://arxiv.org/pdf/2004. 01076.pdf [10] Chady El Mir and Zeina Yassine, Conformal geometric inequalities on the Klein bottle, Conform. Geom. Dyn. 19 (2015), 240–257. [11] , Systolic inequalities and minimal hypersurfaces, Geom. Funct. Anal. 19 (2010), no. 6, 1688–1692. [12] James Hebda, The primitive length spectrum of 2-D tori and generalized Loewner inequalities, Trans. Amer. Math. Soc. 372 (2019), no. 9, 6371–6401. [13] Sergei Ivanov and Mikhail Katz, Generalized degree and optimal Loewner-type inequalities, Israel J. Math. 141 (2004), 221–233. 6 MIKHAILG.KATZANDTAHLNOWIK

[14] Mikhail Katz, Systolic geometry and topology, with an appendix by Jake P. Solomon, Mathematical Surveys and Monographs, 137, American Mathemat- ical Society, Providence, RI, 2007. [15] Mikhail Katz and Stephane Sabourau, Hyperelliptic surfaces are Loewner, Proceedings of the American Mathematical Society 134 (2006), no. 4, 1189– 1195. [16] Yevgeny Liokumovich, Alexander Nabutovsky, and Regina Rotman, Lengths of three simple periodic geodesics on a Riemannian 2-sphere, Math. Ann. 367 (2017), no. 1–2, 831–855. [17] Stephane Sabourau, Isosystolic three surfaces critical for slow metric variations, Geom. Topol. 15 (2011), no. 3, 1477–1508. [18] Bal´azs Csik´os and M´arton Horv´ath, Harmonic manifolds and tubes, J. Geom. Anal. 28 (2018), no. 4, 3458–3476.

M. Katz, Department of Mathematics, Bar Ilan University, Ramat Gan 5290002 Israel E-mail address: [email protected] T. Nowik, Department of Mathematics, Bar Ilan University, Ramat Gan 5290002 Israel E-mail address: [email protected]