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and projective invariants

B. Najafi and A. Tayebi

Abstract.In this paper, we define a new projective invariant and call it Wf-curvature. We prove that a Finsler manifold with dimensionn≥3 is of constant flag curvature if and only if itsWf-curvature vanishes. Various kinds of projectively flatness of Finsler metrics and their equivalency on Riemannian metrics are also studied.

M.S.C. 2010: 53B40, 53C60.

Key words: Projective transformation; scalar flag curvature.

1 Introduction

One of the fundamental problems in Finsler geometry is to study and characterize Finsler metrics of constant flag curvature. The best well-known result towards this question is due to Akbar-Zadeh, which classified compact Finsler manifolds with non- positive constant flag curvature [3]. In a 25 year research, initiated by famous Yasuda- Shimada’s theorem [16] and finished by Bao-Robless-Shen’s theorem [7], Randers metrics of constant flag curvature have been classified.

On the other hand, there are some well-known projective invariants of Finsler metrics namely, Douglas curvature [5][6][10], Weyl curvature, generalized Douglas - Weyl curvature [4][13] and another projective invariant which is due to Akbar-Zadeh [1]. In [21], Weyl introduces a projective invariant for Riemannian metrics. Then Douglas extendes Weyl’s projective invariant to Finsler metrics [10]. Finsler metrics with vanishing projective Weyl curvature are calledWeyl metrics. In [18], Z. Szab´o proves that Weyl metrics are exactly Finsler metrics of scalar flag curvature.

In [3], Akbar-Zadeh introduces the non-Riemannian quantityHwhich is obtained from the mean Berwald curvature by the covariant horizontal differentiation along geodesics. This is a positively homogeneous scalar function of degree zero on the slit tangent bundle, and recently has been studied [11][12]. Akbar-Zadeh proves that for a Weyl manifold of dimensionn 3 , the flag curvature is constant if and only if H= 0. The natural question is: Is there any projectively invariant quantity which characterizes Finsler metrics of constant flag curvature?

Balkan Journal of Geometry and Its Applications, Vol.15, No.2, 2010, pp. 90-99 (electronic version);

pp. 82-91 (printed version).

°c Balkan Society of Geometers, Geometry Balkan Press 2010.

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In this paper, using Akbar-Zadeh’s method in [1], we define a new projective invari- ant and call itWf-curvature (see the equation (3.14)). We show that theWf-curvature is another candidate for characterizing Finsler metrics of constant flag curvature.

More precisely, we prove the following

Theorem 1.1. Let (M, F)be a Finsler manifold with dimension n≥3. ThenF is of constant flag curvature if and only if fW = 0.

By Akbar-Zadeh’s theorem and Theorem 1.1, we have the following

Corollary 1.1. Let (M, F) be a Finsler manifold with dimension n 3. Suppose thatF is of scalar flag curvature. Then H= 0 if and only if Wf= 0.

Throughout this paper, we use the Berwald connection on Finsler manifolds [19][20]. The h- and v- covariant derivatives of a Finsler tensor field are denoted by “|” and “, ” respectively.

2 Preliminaries

Let M be an n-dimensional C manifold. Denote by TxM the tangent space at x∈M, and byT M =x∈MTxM the tangent space ofM. AFinsler metriconM is a functionF :T M [0,∞) which has the following properties: (i)F isConT M0; (ii)F is positively 1-homogeneous on the fibers of tangent bundleT M, and (iii) for eachy∈TxM, the following quadratic formgy onTxM is positive definite,

gy(u, v) := 1 2

£F2(y+su+tv)¤

|s,t=0, u, v∈TxM.

Given a Finsler manifold (M, F), then a global vector field G is induced by F on T M0, which in a standard coordinate (xi, yi) forT M0 is given by

G=yi

∂xi 2Gi(x, y)

∂yi,

whereGi(x, y) are local functions on T M0 satisfying Gi(x, λy) =λ2Gi(x, y), for all λ >0. FunctionsGi are given by

(2.1) Gi :=1

4gil{2∂gjl

∂xk −∂gjk

∂xl }yjyk,

where gij is the vertical Hessian of F2/2 and gij denotes its inverse. G is called the associated spray to (M, F). The projection of an integral curve of G is called a geodesic in M. In local coordinates, a curve c(t) is a geodesic if and only if its coordinates (ci(t)) satisfy ¨ci+ 2Gi( ˙c) = 0 [14].

For a vectorvivertical and horizontal covariant derivative with respect to Berwald connection are given by

v,ki = ˙kvi, vi|k=dkvi+Gijkvj,

wheredk=k−Gmk˙m,k= ∂xk, ˙k =∂yk,Gik= ˙kGi andGijk= ˙jGik.

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In [1], Akbar-Zadeh cosideres a non-Riemannian quantity H which is obtained from the mean Berwald curvature by the covariant horizontal differentiation along geodesics. This is a positively homogeneous scalar function of degree zero on the slit tangent bundle. The quantityH=Hijdxi⊗dxjis defined as the covariant derivative ofE along geodesics, whereEij = 12˙mGmij [12]. More preciselyHij :=Eij|mym. In local coordinates, we have

2Hij = ym 4Gk

∂yi∂yj∂yk∂xm2Gm 4Gk

∂yi∂yj∂yk∂ym

∂Gm

∂yi

3Gk

∂yj∂yk∂ym−∂Gm

∂yj

4Gk

∂yi∂yk∂ym. The Riemannian curvature tensor of Berwald connection are given by

Kihjk=djGihk+GmhkGimj−dkGihj+GmhjGimk. LetKjki =Ki0jkandKki =Ki0k. Then we have

Kjki = 1

3{∂˙jKki−∂˙kKji}.

Then, the Riemann curvature operator of Berwald connection aty∈TxM is defined byKy=Kikdxk∂xi|x:TxM →TxM, which is a family of linear maps on tangent spaces. The flag curvature in Finsler geometry is a natural extension of the sectional curvature in Riemannian geometry, which is first introduced by L. Berwald [8]. For a flagP = span{y, u} ⊂TxM with flagpoley, theflag curvatureK=K(P, y) is defined by

K(P, y) := gy(u,Ky(u))

gy(y, y)gy(u, u)gy(y, u)2.

WhenFis Riemannian,K=K(P) is independent ofy∈P, which is just the sectional curvature ofP in Riemannian geometry. We say that a Finsler metricF isof scalar curvatureif for anyy∈TxM, the flag curvatureK=K(x, y) is a scalar function on the slit tangent space T M0. IfK =constant, then F is said to be of constant flag curvature.

The projective Weyl curvature is defined as follows Wjkli :=Kjkli 1

1−n2 n

−δji( ˜Kkl−K˜lk)−δkiK˜jl+δliK˜jk−yi˙j( ˜Kkl−K˜lk)o where ˜Kjk:=nKjk+Kkj+yr˙jKkr. As it is well known, a Finsler metric is of scalar flag curvature if and only ifWjkli = 0.

3 C-projective Weyl curvature

Letφ:Fn→F¯n be a diffeomorphism. We callφa projective mapping if there exists a positive homogeneous scalar functionP(x, y) of degree one satisfying

G¯i=Gi+P yi.

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In this case,P is called the projective factor ([17]). Under a projective transformation with projective factor P, the Riemannian curvature tensor of Berwald connection change as follows

(3.1) K¯ihjk =Kihjk+yi˙hQjk+δhiQjk+δij˙hQk−δik˙hQj,

where Qi =diP −P Pi and Qij = ˙iQj −∂˙jQi. A projective transformation with projective factorP is said to be C-projectiveifQij = 0.

Let X be a projective vector field on a Finsler manifold (M, F). Let the vector fieldX in a local coordinate (xi) on M be written in the formX =Xi(x)∂i. Then the complete lift ofX is denoted by ˆX and locally defined by ˆX=Xii+yjjXi˙i. Suppose that £Xˆ stands for Lie derivative with respect to the complete lift of X.

Then we have

£XˆGi =P yi,

£XˆGik=δikP+yiPk,

£XˆGijk=δjiPk+δikPj+yiPjk, (3.2) £XˆGijkl=δjiPkl+δkiPjl+δliPkj+yiPjkl,

(3.3) £XˆKjkli =δij(Pl|k−Pk|l) +δilPj|k−δkiPj|l+yi˙j(Pl|k−Pk|l).

SinceQij =Pi|j−Pj|i, we have

(3.4) £XˆKjkli =δjiQlk+δilPj|k−δkiPj|l+yi˙jQlk. We have

(3.5) ˙jPk|l=Pjk|l−PrGrjkl. Contractingiandk in (3.4), we get

(3.6) £XˆKjl=Pl|j−nPj|l+Pjl|sys. Consequently

(3.7) £Xˆ(yr˙lKjr) =−(n+ 1)Pjl|sys. Hence

(3.8) Pjl|sys= 1

n+ 1L( ˆX)(yr˙lKjr), and

(3.9) £Xˆ(Kjl+ 1

n+ 1yr˙lKjr) =Pl|j−nPj|l,

(3.10) £Xˆ(Klj+ 1

n+ 1yr˙jKlr) =Pj|l−nPl|j.

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Using (3.9) and (3.10), one can obtain (3.11) Pj|l= 1

1−n2£Xˆ

n

Klj+ 1

n+ 1yr˙jKlr+nKjl+ n

n+ 1yr˙lKjr

o . IfQij = 0, then (3.4) reduces to the following

(3.12) £XˆKjkli =δilPj|k−δkiPj|l.

Using (3.11) and eliminatingPj|lfrom (3.12), we are led to the following tensor Wfjkli :=Kjkli 1

1−n2δlin

K˜jk+ n

n+ 1yr( ˙kKjr−∂˙jKkr)o

+ 1

1−n2δkin

K˜jl+ n

n+ 1yr( ˙lKjr−∂˙jKlr)o . (3.13)

Sinceyjyr˙kKjr= 0, if we put Wfki :=fWjkli yjyl, then we have (3.14) Wfik =Kik 1

1−n2 n

yiK˜0k−δikK˜00

o .

The tensorfWki is said to beC-projective Weyl curvatureor Wf-curvature. According to the way we constructfW, it is easy to see thatWfisC-projective invariant tensor. A Finsler metricF is calledC-projective Weyl metricif itsC-projective Weyl-curvature vanishes. First, we prove that the class of Weyl metrics contains the class of C- projective Weyl metrics.

Theorem 3.1. Let F be aC-projective Weyl metric. ThenF is a Weyl metric.

Proof. By assumption, we have the following

(3.15) Kki 1

1−n2 n

yiK˜0k−δkiK˜00

o

= 0.

Contracting (3.15) withyi implies that

(3.16) F2K˜0k−ykK˜00= 0.

Hence

(3.17) K˜0k=F−2ykK˜00. Plugging (3.17) into (3.15), we get

(3.18) Kki = 1

1−n2K˜00hik,

which means thatF is of scalar flag curvature. Hence,F is a Weyl metric. ¤

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4 Proof of Theorem 1.1

To prove Theorem 1.1, we need to find theWf-curvature of Weyl metrics.

Proposition 4.1. Let F be a Finsler metric of scalar flag curvature λ. Then fW- curvature is given by

(4.1) Wfki =1

3F2yiλk, whereλk := ˙kλ.

Proof. By assumption, the Riemannian curvature of Berwald connection is in the following form.

Kjkli = λ(δikgjl−δligjk) +λjFkiFl−δilFk) +1

3F2(hikλjl−hilλjk) + 1

3λlF(2δikFjijFk−gjk`i)

1

3F λk(2δilFjijFl−gjl`i).

(4.2)

whereλij = ˙jλi. Hence, we have

(4.3) Kki =λF2hik.

Then, we get the following relations.

Kjl = (n1)(λgjl+F Flλj) +n−2

3 (F2λjl+ 2F Fjλl), K00=λ(n−1)F2, K˜00=λ(n21)F2,

Kk0=λ(n−1)F Fk+2n1 3 F2λk, K0k =λ(n−1)F Fk+n−2

3 F2λk, K˜0k = (n21)(λF Fk+1

3F2λk).

(4.4)

Plugging (4.3) and (4.4) into (3.14), we get the result. ¤ Lemma 4.1. Let (M, F) be a C-projective Weyl manifold with dimension n 3.

ThenF is of constant flag curvature.

Proof. By Theorem 3.1 and Proposition 4.1, we have Wfki =1

3F2yiλk.

From assumption, we getλk = 0. It means thatF is of isotropic flag curvature. The

result follows by Schur’s Lemma. ¤

Now, let us consider the caseF being of constant flag curvature.

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Lemma 4.2. Let F be a Finsler metric of constant flag curvature K=λ. Then F isC-projective Weyl metric.

Proof. IfF is of constant flag curvatureλ, then (4.2) reduces to the following (4.5) Kjkli =λ(gjlδik−gjkδli).

Hence

(4.6) Kjl=λ(1−n)gjl, K˜jk=λ(1−n2)gjl.

Plugging (4.6) into (3.13), we obtainfWjkli = 0 and consequentlyfWki= 0. ¤

5 Reduction in Riemannian manifolds

As mentioned before, in Finsler metricsFn of scalar flag curvature with (n3), we have this equivalenceWf= 0 if and only ifH= 0. ObservingC-projective invariancy ofWf-curvature, one can conjecture thatH-curvature must beC-projective invariant too. Here, we prove that this is true. By definition,Hij =Eij|sys. Under a projective transformation with the projective factorP, we have the following relations:

E¯ij = Eij+n+ 1 2 Pij, yld¯l = yldl2P ym˙m,

E¯mjG¯mi = EmjGmi +P Eij+n+ 1

2 (PmjGmi +P Pij).

Now, we can prove the following

Proposition 5.1. H-curvature is C-projective invariant.

Proof. Under a projective transformation, we have H¯ij = E¯ij|lyl

= yld¯lE¯ij−E¯mjG¯mi −E¯imG¯mj

= (yldlE¯ij2P ym˙mE¯ij)−E¯mjG¯mi −E¯imG¯mj

= yldlEij+n+ 1

2 yldlPij+ 2P Eij+ (n+ 1)P Pij−E¯mjG¯mi −E¯imG¯mj

= yldlEij−EmjGmi −EimGmj +n+ 1

2 (yldlPij−PmjGmi −PimGmj )

= Hij+n+ 1

2 (yldlPij−PmjGmi −PimGmj ).

(5.1)

On the other hand, we have

yl˙iQjl = yldlPij−PmjGmi −yldjPil

= yldlPij−PmjGmi −PmiGmj (5.2)

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Plugging (5.2) into (5.1) yields

(5.3) H¯ij =Hij+n+ 1

2 yl˙iQjl.

We deal withC-projective mapping, i.e.,Qij = 0. Hence ¯Hij =Hij. This completes

the proof. ¤

A locally projectively flat Finsler manifold (M, F) with the projective factorP is said to be locallyC-projectively flat if P satisfies Qij = 0, this means F is locally C-projectively related to a locally Minkowskian metric.

Example. Let Θ be the Funk metric on the Euclidean unit ballBn(1) , i.e., Θ(x, y) :=

p|y|2(|x|2|y|2−< x, y >2)+< x, y >

1− |x|2 , y∈TxBn(1)'Rn, where<, >and|.|denotes the Euclidean inner product and norm onRn, respectively.

For a constant vectora∈Rn, letF be the Finsler metric given by (5.4) F :={1+< a, x >+< a, y >

Θ }{Θ + Θxkxk}.

In [15], Shen proves thatF is projectively flat with projective factorP = Θ. A direct computation shows thatQij = 0. Hence, F is locallyC-projectively flat. Moreover, Shen proves thatF is of constant flag curvature K= 0.

Every locally Minkowskian metric has vanishing H-curvature. It is well known that every locally projectively flat Finsler metric is of scalar flag curvature. In the case of locallyC-projectively flat Finsler metrics we have the following

Corollary 5.1. Let F be a locally C-projectively flat Finsler metric. Then F is of constant flag curvature.

In studying the subgroups of the group of projective transformations, Akbar- Zadeh considers projective vector fields satisfyingPij = 0 and calls this kind of vector fields, restricted projective vector field [1]. The condition Pij = 0 means that the projective factorP is linear, which is always true in Riemannian manifolds. Hence, in Riemannian manifolds, every projective transformation is restricted.

Let us define locally restricted projectively flatness similar toC-projectively flat- ness. Note that Finsler metric given in Example 1 is not locally restricted projectively flat. In fact, a restricted projective vector field withP =ai(x)yi isC-projective vec- tor field, ifai(x) is gradient, that isP =for some scalar function on the underlying manifold.

Using (3.11) and eliminatingPj|lfrom (3.4), Akbar-Zadeh introduces the following tensor

Wijkl:=Kijkl 1 n21

n

δki(nKjl+Klj)−δli(nKjk+Kkj) o

1

n+ 1δij(Kkl−Klk).

(5.5)

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Under aC-projective mapping, we have

(5.6) Wijkl=Wijkl+ 2δki˙lQjil˙jQk.

This means thatWijkl is not aC-projective invariant. In fact,Wijkl is a restricted projective invariant. We callWijklrestricted projective Weyl-curvature. The geomet- ric importance of the restricted projective Weyl-curvature is to characterize Finsler metrics of constant flag curvature, i.e., a Finsler metricFn with (n3) is of constant flag curvature if and only ifF has vanishing restricted projective Weyl-curvature ([2]

page 209).

Now letF be a Riemannian metric. By Beltrami’s well-known theorem, locally projectively flat Riemannian manifolds are exactly Riemannian manifolds of constant sectional curvature. Summarizing up, we get the following reduction theorem in Riemannian manifolds.

Theorem 5.1. Let (M, F)be Riemannian manifold with dimensionn≥3. Then the following are equivalent.

1. F is locally projectively flat.

2. F is locally restricted projectively flat.

3. F is locallyC-projectively flat.

This is not true in generic Finslerian manifolds. The non-equivalence between these kind of projective mappings in Finsler manifolds reveals the complexity of Finsler spaces.

Acknowledgments. The authors express their sincere thanks to Professors H. Akbar-Zadeh, Z. Shen and referees for their valuable suggestions and comments.

References

[1] H. Akbar-Zadeh, Champ de vecteurs projectifs sur le fibre unitaire, J. Math.

Pures Appl. 65 (1986), 47-79.

[2] H. Akbar-Zadeh,Initiation to Global Finslerian GeometryNorth-Holand Math- ematical Library, Vol 68 (2006).

[3] H. Akbar-Zadeh,Sur les espaces de Finsler A courbures sectionnelles constantes Acad. Roy. Belg. Bull. Cl. Sci. 74 (1988), 271-322.

[4] S. B´acs´o and I. Papp, A note on generalized Douglas space, Periodica Mathe- maticia Hungarica Vol. 48 (1-2), 2004, pp. 181-184.

[5] V. Balan, M. Crane, V. Patrangenaru and X. Liu, Projective shape manifolds and coplanarity of landmark configurations. A nonparametric approach, Balkan J. Geom. Appl. 14, 1 (2009), 1-10.

[6] S. B´acs´o and M. Matsumoto,On Finsler spaces of Douglas type, A generalization of notion of Berwald space, Publ. Math. Debrecen. 51 (1997), 385-406.

[7] D. Bao, C. Robles and Z. Shen, Zermelo navigation on Riemannian manifolds, J. Diff. Geom. 66 (2004), 391-449.

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[8] L. Berwald, Uber Parallel¨ubertragung in R¨aumen mit allgemeiner Massbestim-¨ mung, Jber. Deutsch. Math.-Verein. 34(1926), 213-220.

[9] B. Bidabad, Complete Finsler manifolds and adapted coordinates, Balkan J.

Geom. Appl. 14, 1 (2009), 21-29.

[10] J. Douglas,The general geometry of path, Ann. Math. 29(1927-28), 143-168.

[11] X. Mo, On the non-Riemannian quantity H of a Finsler metric, Differential Geometry and its Application, 27 (2009), 7-14.

[12] B. Najafi, Z. Shen and A. Tayebi ,Finsler metrics of scalar flag curvature with special non-Riemannian curvature properties, Geom. Dedicata. 131 (2008), 87- 97.

[13] B. Najafi, Z. Shen and A. Tayebi,On a projective class of Finsler metrics, Publ.

Math. Debrecen. 70 (2007), 211-219.

[14] Z. Shen,Differential Geometry of Spray and Finsler Spaces, Kluwer Academic Publishers, Dordrecht, 2001.

[15] Z. Shen,Projectively flat Finsler metrics of constant flag curvature, Transactions of the American Mathematical Society, 355, 4 (2003), 1713-1728

[16] H. Shimada,Short review of Yasuda-Shimada Theorem and related topics, Peri- odica Mathematica Hungarica Vol. 48 (12), 2004, 17-24

[17] S.P. Singh, Projective motion in bi-recurrent Finsler space, Diff. Geom. Dyn.

Syst. 12 (2010), 221-227.

[18] Z. Szab´o,Ein Finslerscher Raum ist gerade dann von skalarer Kr¨ummung, wenn seine Weyl sche ProjectivKr¨ummung verschwindet, Acta Sci. Math. 39 (1977), 163-168.

[19] A. Tayebi, E. Azizpour and E. Esrafilian,On a family of connections in Finsler geometry, Publ. Math. Debrecen. 72 (2008), 1-15.

[20] A. Tayebi and B. Najafi,Shen’s Processes on Finslerian Connections, Bull. Iran.

Math. Soc. 36 (2010), 1-17.

[21] H. Weyl,Zur Infinitesimal geometrie, G¨ottinger Nachrichten. (1921), 99-112.

Authors’ addresses:

Behzad Najafi

Faculty of Science, Department of Mathematics, Shahed University, Tehran, Iran.

E-mail: [email protected] Akbar Tayebi

Faculty of Science, Department of Mathematics, Qom University, Qom, Iran.

E-mail: [email protected]

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