ON RANDERS CHANGE OF GENERALIZED mth ROOT METRIC

Similar documents
On Einstein Kropina change of m-th root Finsler metrics

WITH SOME CURVATURE PROPERTIES

On Randers-Conformal Change of Finsler Space with Special (α, β)-metrics

RANDERS METRICS WITH SPECIAL CURVATURE PROPERTIES

On a Class of Locally Dually Flat Finsler Metrics

ON THE CONSTRUCTION OF DUALLY FLAT FINSLER METRICS

Projectively Flat Fourth Root Finsler Metrics

Bulletin of the Transilvania University of Braşov Vol 7(56), No Series III: Mathematics, Informatics, Physics, 1-12

arxiv: v1 [math.dg] 21 Dec 2017

Conformal transformation between some Finsler Einstein spaces

On Douglas Metrics. Xinyue Chen and Zhongmin Shen. February 2, 2005

On a class of Douglas metrics

On homogeneous Randers spaces with Douglas or naturally reductive metrics

arxiv: v1 [math.dg] 12 Feb 2013

Research Article On a Hypersurface of a Finsler Space with Randers Change of Matsumoto Metric

Acta Mathematica Academiae Paedagogicae Nyíregyháziensis 25 (2009), ISSN

On a class of stretch metrics in Finsler Geometry

Acta Mathematica Academiae Paedagogicae Nyíregyháziensis 24 (2008), ISSN

The Fundamental Basis Theorem of Geometry from an algebraic point of view

Alireza Kamel Mirmostafaee

Strictly convex functions on complete Finsler manifolds

NEW LIFTS OF SASAKI TYPE OF THE RIEMANNIAN METRICS

PAijpam.eu NONHOLONOMIC FRAMES FOR A FINSLER SPACE WITH GENERAL (α, β)-metric

RIGIDITY OF QUASI-EINSTEIN METRICS

ON RANDERS SPACES OF CONSTANT CURVATURE

On the rectifiability condition of a second order differential equation in special Finsler spaces

The Distribution of the Covariance Matrix for a Subset of Elliptical Distributions with Extension to Two Kurtosis Parameters

FINSLERIAN HYPERSURFACES AND RANDERS CONFORMAL CHANGE OF A FINSLER METRIC

On Berwald Spaces which Satisfy the Relation Γ k ij = p k g ij for Some Functions p k on TM

Lagrange Spaces with β-change

SOME INVARIANTS CONNECTED WITH EULER-LAGRANGE EQUATIONS

On a Class of Weakly Berwald (α, β)- metrics of Scalar flag curvature

arxiv: v1 [math.dg] 21 Oct 2015

The Explicit Construction of Einstein Finsler Metrics with Non-Constant Flag Curvature

International Journal of Pure and Applied Mathematics Volume 48 No , A STUDY OF HYPERSURFACES ON SPECIAL FINSLER SPACES

HYPERSURFACE OF A FINSLER SPACE WITH DEFORMED BERWALD-MATSUMOTO METRIC

Algebraic Montgomery-Yang problem: the log del Pezzo surface case

ON HYPER SURFACE OF A FINSLER SPACE WITH AN EXPONENTIAL - METRIC OF ORDER M

P. Mutlu and Z. Şentürk ON WALKER TYPE IDENTITIES LOCALLY CONFORMAL KAEHLER SPACE FORMS

ON REGULARITY, TRANSITIVITY, AND ERGODIC PRINCIPLE FOR QUADRATIC STOCHASTIC VOLTERRA OPERATORS MANSOOR SABUROV

i ij j ( ) sin cos x y z x x x interchangeably.)

Four-vector, Dirac spinor representation and Lorentz Transformations

Some Open Problems in Finsler Geometry

ON SOME MATRIX INEQUALITIES. Hyun Deok Lee. 1. Introduction Matrix inequalities play an important role in statistical mechanics([1,3,6,7]).

arxiv: v1 [math.gm] 20 Jul 2017

SUBTANGENT-LIKE STATISTICAL MANIFOLDS. 1. Introduction

NEW TOOLS IN FINSLER GEOMETRY: STRETCH AND RICCI SOLITONS

Acta Mathematica Academiae Paedagogicae Nyíregyháziensis 24 (2008), ISSN

arxiv: v1 [math.fa] 13 Dec 2011

THE TANGENT BUNDLES and HARMONICITY 1. Dedicated to Professor Gh.Gheorghiev on the occasion of his 90-th birthday.

A SIMPLE METHOD FOR FINDING THE INVERSE MATRIX OF VANDERMONDE MATRIX. E. A. Rawashdeh. 1. Introduction

The Johns Hopkins University Press is collaborating with JSTOR to digitize, preserve and extend access to American Journal of Mathematics.

Time-Periodic Solutions of the Einstein s Field Equations

Chapter 6 1-D Continuous Groups

On isometries of Finsler manifolds

Block designs and statistics

ON SEQUENCES OF NUMBERS IN GENERALIZED ARITHMETIC AND GEOMETRIC PROGRESSIONS

COHOMOLOGY OF FOLIATED FINSLER MANIFOLDS. Adelina MANEA 1

The Stress Distribution in the Composite Materials with Locally Curved Fibers

Explicit solution of the polynomial least-squares approximation problem on Chebyshev extrema nodes

PROCEEDINGS OF THE YEREVAN STATE UNIVERSITY

Pattern Recognition and Machine Learning. Learning and Evaluation for Pattern Recognition

Homotopy Analysis Method for Solving Fuzzy Integro-Differential Equations

Homogeneous Geodesics of Left Invariant Randers Metrics on a Three-Dimensional Lie Group

STRONG LAW OF LARGE NUMBERS FOR SCALAR-NORMED SUMS OF ELEMENTS OF REGRESSIVE SEQUENCES OF RANDOM VARIABLES

DIFFERENTIAL EQUATIONS AND RECURSION RELATIONS FOR LAGUERRE FUNCTIONS ON SYMMETRIC CONES

arxiv: v1 [math.dg] 5 Jan 2016

NON-COMMUTATIVE GRÖBNER BASES FOR COMMUTATIVE ALGEBRAS

Intelligent Systems: Reasoning and Recognition. Perceptrons and Support Vector Machines

ON THE TWO-LEVEL PRECONDITIONING IN LEAST SQUARES METHOD

Lie Algebra of Unit Tangent Bundle in Minkowski 3-Space

A new type of lower bound for the largest eigenvalue of a symmetric matrix

A Study on B-Spline Wavelets and Wavelet Packets

Generalized AOR Method for Solving System of Linear Equations. Davod Khojasteh Salkuyeh. Department of Mathematics, University of Mohaghegh Ardabili,

Polygonal Designs: Existence and Construction

On the geometry of higher order Lagrange spaces.

A NEW CHARACTERIZATION OF THE CR SPHERE AND THE SHARP EIGENVALUE ESTIMATE FOR THE KOHN LAPLACIAN. 1. Introduction

Poornima University, For any query, contact us at: , 18

arxiv: v1 [math.co] 19 Apr 2017

Certain Subalgebras of Lipschitz Algebras of Infinitely Differentiable Functions and Their Maximal Ideal Spaces

A Geometric Characterization of Homogeneous Production Models in Economics

Bulletin of the Iranian Mathematical Society

GENERALIZED QUATERNIONIC STRUCTURES ON THE TOTAL SPACE OF A COMPLEX FINSLER SPACE

Linear Programming. Murti V. Salapaka Electrical Engineering Department University Of Minnesota, Twin Cities

A note on the realignment criterion

Monochromatic metrics are generalized Berwald

AN ITERATIVE MAXIMUM EIGENVALUE METHOD FOR SQUARED DISTANCE SCALING 1. INTRODUCTION

Generalized binomial expansion on Lorentz cones

LIOUVILLE THEOREM AND GRADIENT ESTIMATES FOR NONLINEAR ELLIPTIC EQUATIONS ON RIEMANNIAN MANIFOLDS

RIEMANN COMPATIBLE TENSORS. 1. Introduction

AN ESTIMATE FOR BOUNDED SOLUTIONS OF THE HERMITE HEAT EQUATION

SOME RESULTS ON THE GEOMETRY OF MINKOWSKI PLANE. Bing Ye Wu

THE POLYNOMIAL REPRESENTATION OF THE TYPE A n 1 RATIONAL CHEREDNIK ALGEBRA IN CHARACTERISTIC p n

On some special vector fields

On normalized Ricci flow and smooth structures on four-manifolds with b + =1

#A62 INTEGERS 16 (2016) REPRESENTATION OF INTEGERS BY TERNARY QUADRATIC FORMS: A GEOMETRIC APPROACH

On Sum and Restriction of Hypo-EP Operators

}, (n 0) be a finite irreducible, discrete time MC. Let S = {1, 2,, m} be its state space. Let P = [p ij. ] be the transition matrix of the MC.

Rationality Problems of the Principles of Equivalence and General Relativity

A note on the multiplication of sparse matrices

Transcription:

Khayya J. Math. 5 09, no., 69 78 DOI: 0.03/kj.08.7578 ON RANDERS CHANGE OF GENERALIZED TH ROOT METRIC MANOJ KUMAR Counicated by B. Mashayekhy Abstract. In the present paper, we find a condition under which a Finsler space with Randers change of generalized th root etric is projectively related to an th root etric. Then we find a condition under which Randers change of generalized th root Finsler etric is locally projectively flat and also find a condition for locally dually flatness.. Introduction In 9, Randers 6 introduced a special class of Finsler space defined by F = F + β, F is a Rieannian etric and β = b i xy i is a one-for. Matsuoto studied Randers spaces and generalized Randers spaces in which F is Finslerian. The theory of th root etrics has been developed by Matsuoto and Shiada see 5 and 7 and applied to ecology by Antonelli and studied by any authors see 0,,, 3. Recent studies show that th root Finsler etrics plays a very iportant role in physics, space-tie, general relativity as well as in unified gauge field theory see. In 9, Tayebi and Najafi characterized locally dually flat and Antonelli th root etrics. Recently, Tayebi, Peyghan, and Shahbazi Nia 0 has introduced generalized th root Finsler etrics in which they studied locally dually flatness of generalized th root Finsler etrics and found a condition under which a generalized th root etric is projectively related to an th root etric. Throughout this paper, we call the Finsler etric F as transfored th root etric and M n, F = F n as transfored Finsler space. We restrict ourselves to >, throughout the paper and also the quantities corresponding to the Date: Received: 9 July 08; Revised: Septeber 08; Accepted: 0 October 08. 00 Matheatics Subject Classification. Priary 53B0; Secondary 53C60. Key words and phrases. Finsler space; Randers change of generalized th root etrics; projectively related etrics; locally projectively flat etric; locally dually flat etric. 69

70 MANOJ KUMAR transfored Finsler space F n will be denoted by putting bar on the top of that quantity. In this paper, we obtain the condition under which the transfored Finsler space is projectively related with the given Finsler space. Also we find the condition under which the transfored Finsler space is locally projectively flat and locally dually flat.. Preliinaries Let M n be an n-diensional C -anifold, and let T x M denote the tangent space of M n at x. The tangent bundle T M is the union of tangent spaces, T M := x M T xm. We denote the eleents of T M by x, y, x = x i is a point of M n and y T x M, called supporting eleent. We denote T M 0 = T M \ {0}. Definition.. A Finsler etric on M n is a function F : T M 0, with the following properties: i F is C on T M 0, ii F is positively -hoogeneous on the fibers of tangent bundle T M, and iii the Hessian of F with eleent g ij = F is positive definite on T M y i y j 0. The pair M n, F = F n is called a Finsler space. F is called the fundaental function, and g ij is called the fundaental etric tensor of the Finsler space F n. The noralized supporting eleent l i and angular etric tensor h ij of F n are defined, respectively, as: l i = F y i and h ij = F F y i y j.. Let F = A be an th root Finsler etric, A is given by A := a i i...i x y i y i... y i, with a i...i is syetric in all its indices 7. The generalized th root etric is defined as F = F + B. Here F is called an associated th root etric of the generalized th root etric F 8. Consider the transfored Finsler etric F = F + B + C,. B = b ij xy i y j and C = c i xy i is a one-for on the anifold M n. This transfored etric F is called Randers change of generalized th root etric. Clearly F is also a Finsler etric on M n. Let, A i = A y i, A ij = A y i y j, B i = B y i, C i = C y i, A x i = A x i, A 0 = A x iy i, B x i = B x i, B 0 = B x iy i, C x i = C x i, C 0 = C x iy i.

ON RANDERS CHANGE OF GENERALIZED TH ROOT METRIC 7 3. Fundaental etric tensor with Randers change of generalized th root etric Fro., we have F = A + B + C + C A + B. 3. Differentiating equation 3. with respect to y i yields F = A y i A A A i + b ij y j + CC i + C i A i + b ij y j C + B +. A + B 3. Again, differentiating equation 3. with respect to y j yields F = y i y j A A i A j + A A ij + b ij + C i C j C i A A j + b jk y k + A + B { } A + B A A i A j + A A ij + b ij C + A + B C j A + B A A i + b ij y j + A + B C A A i + b ij y j A A j + b ij y i. A + B 3 Therefore, g ij = A A i A j + A A ij + b ij + C i C j C i A A j + b jk y k + A + B { +A + B A A i A j + A A ij + b ij C } + C j A A i + b ij y j CA + B 3 A A i + b ij y j A A j + b ij y i. The etric tensor of Finsler space with Randers change of generalized th root etric is given by C ḡ ij = gˆ ij + + C i C j + C id j + C j D i D i D j C, 3.3 A + B A + B A + B 3/

7 MANOJ KUMAR and gˆ ij = g ij + b ij, D i = A A i + b ij y j, D j = A A j + b ij y i g ij = A AA ij + A i A j. Proposition 3.. The covariant etric tensor ḡ ij of Randers change of generalized th root etric is given as: C ḡ ij = gˆ ij + + C i C j + C id j + C j D i D i D j C A + B A + B A + B. 3/. Spray coefficients of Randers change of generalized th root etric The geodesics of a Finsler space F n are given by the following syste of equations: d x i dt + Gi x, dx = 0, i =,,..., n, dt G i = gil { F x k y l y k F x l }. are called the spray coefficients of F n. Two Finsler etrics F and F on a anifold M n are called projectively related if there is a scalar function P x, y defined on T M 0 such that Ḡi = G i + P y i, Ḡ i and G i are the geodesic spray coefficients of F n and F n, respectively. In other words, two etrics F and F are called projectively related if any geodesic of the first is also geodesic for the second and vice versa. The spray coefficients of Randers change of generalized th root Finsler space F n is given by Ḡ i = ḡil { x k y l y k x l }.. Lea.. 0. Let A = A ij be an n n invertible and syetric atrix, and let D = D i and E = E i be two nonzero n and n vectors, respectively, such that D i E j = D j E i. Suppose that + A pq D p E q 0. Then, the atrix B = B ij defined by B ij := A ij + D i E j is invertible and B ij := B ij = A ij + A pq D p E q A ki A lj D k E l, atrix A ij denotes the inverse of atrix A ij. Theore.. Let F = A + B + C and F = A be Randers change of generalized th root and an th root Finsler etric on an open subset U R n,

ON RANDERS CHANGE OF GENERALIZED TH ROOT METRIC 73 respectively, A := a i i...i xy i y i... y i, B = b ij xy i y j, and C = c i xy i with. Suppose that the following holds: A A il ζ l + J l + Lb il KC i C l + I il ζ l + J l γ + Lbil I il A i = 0,.3 KC i C l ζ l = B 0l B x l + C l C 0 + CC 0l CC x l, C A + B J l = y k C A + B, x k y l x l γ = KCl A i = { F x ky j y k F x j }, A A ip C p, C l = g lk C k and K, L are constants. Then F is projectively related to F. Proof: By equation., we have F = F + B + C + C Then using Proposition 3., we obtain ḡ ij = gˆ ij + C + C i C j + C id j + C j D i H H gˆ ij = g ij + b ij, A + B.. C D id j H 3,.5 g ij = A AA ij + A i A j,.6 and H = A + B. Fro Lea., we get ḡ ij = ˆ g ij KC i C j + I ij,.7 K is a constant, I ij will be the inverse of the last two ter in equation.5, which easily ay not be calculate explicitly, and gˆ ij = g ij Lb ij = A AAij + yi y j Lb ij,.8 L is a constant and g ij is the inverse of g ij. Then by equations.,., and.7, we have Ḡ i = ˆ gil KC i C l + I il F + B + C + C A + B x k y l y k F + B + C + C A + B x l.

7 MANOJ KUMAR Then fro equation.8, we can write Ḡ i = g il Lb il KC i C l + I il F x k y l yk F x l + g il Lb il KC i C l + I il B x k y l yk B x l + g il Lb il KC i C l + I il C x k y l yk C x l + g il Lb il KC i C l + I il C A + B x k y l y k C A + B x l. That is, Ḡ i = + + g il F x k y l yk F x l KCi C l + Lb il I il F x k y l yk F x l g il Lb il KC i C l + I il B 0l B x l + C l C 0 + CC 0l CC x l g il Lb il KC i C l + I il J l, J l = C A + B x k y l y k C A + B x l. Therefore, Ḡ i = G i γ + Lbil I il KC i C l C i + g il Lb il KC i C l + I il ζ l + g il Lb il KC i C l + I il J l,.9 Putting we have γ = KCl { F x ky y k F }, l x l ζ l = B 0l B x l + C l C 0 + CC 0l CC x l..0 Φ := C i = g ip C p = A A y p C p, A i := A A ip C p,. AAip + yi y p C p = A i + Φy i.. By.8,.9, and., we get Ḡ i = G i + A yl ζ l + J l γ + Lbil I il KC i C l γ + Lbil I il KC i C l A i + A A il ζ l + J l + Φ y i Lb il KC i C l + I il ζ l + J l..3

ON RANDERS CHANGE OF GENERALIZED TH ROOT METRIC 75 If the relation.3 holds, then by.3 the Finsler etric F is projectively related to F. 5. Locally projectively flatness of Randers change of generalized th root etric A Finsler etric is called locally projectively flat if, for any point, there is a local coordinate syste in which the geodesics are straight lines as point sets. It is known that a Finsler etric F x, y on an open doain U R is locally projectively flat if and only if its geodesic coefficients G i take the for G i x, y = P x, yy i, P : T U = U R R is positively hoogeneous with degree one and P x, λy = λp x, y, λ > 0 3. We say that P x, y is the projective factor of F. In other words, a Finsler etric F = F x, y on a anifold M n is said to be locally projectively flat, if and only if F x k y lyk = F x l. Using equation., we have x l = A A x l + B x l A + B + C x l. 5. Fro 5., we get and x k y l = x k = A + B A + B 3 A A x k + B x k + C x k A + B A A y la x k + A A x k y l + B x k y l A + B A Ax k + B x k A Ay l + B y l + C x k y l.5. Let the Finsler etric F be locally projectively flat. Then we have x k y l y k x l = 0. 5.3 Therefore, fro 5., 5., and 5.3, we obtain y x k A + B F k y l x l = A A l A 0 + A A 0l + B 0l A + B A + B 3 A A0 + B 0 A Al + B l + C 0l A A x l + B x l C x l = 0. A + B

76 MANOJ KUMAR Hence, F is locally projectively flat etric if and only if A x l = A A la 0 + A 0l + A B0l A + B A Al + B l + C 0l C x l A A 0 + A B0 A + B B xla. 5. Thus, we have the following result. Theore 5.. Let F = A + B + C be a Randers change of generalized th root Finsler etric on a anifold M n. Then, F is a locally projectively flat etric if and only if equation 5. satisfied. 6. Locally dually flatness of Randers change of generalized th root etric In Finsler geoetry, Shen extended the notion of locally dually flatness for Finsler etrics. A Finsler etric F = F x, y on a anifold M n is said to be locally dually flat, if at any point there is a standard coordinate syste x i, y i in T M such that x k y l y k = x l. Every locally Minkowskian etric is locally dually flat. Using equation., we have x l = A Ax l + B x l + CC x l + Fro 6., we get x k = A Ax k + B x k + CC x k + and = x k y l A Ax k y l + x + A + B + B x k y l + CCk y l + C lc x k A + B + C x k y l A + B + C x k { CA A x l + CB x l + C x l A + B. 6. A + B A Al A x k CA A x k + CB x k A + B CA + C x k A + B CA Ax k y l Al A x k + + } A Ax kc l + C l B x k + CB x k y l CA Ax k + CB x k A A + B A Al + B l A l + B l. 6. A + B Let the Finsler etric F be locally dually flat. Then we have x k y l y k x l = 0. 6.3

ON RANDERS CHANGE OF GENERALIZED TH ROOT METRIC 77 Therefore, fro 6., 6., and 6.3, we obtain y k F = x k y l x l A A0l + + B 0l + CC 0l + C l C 0 =0. { + A + B A Al A 0 CA CA A0l Al A 0 + + } A A0 C l + C l B 0 + CB 0l A + B 3 CA A0 + CB 0 + C 0l A + B + C 0 A A l + B l A + B A Ax l B x l CC x l CA A x l + CB x l C x l A + B Therefore, F is locally dually flat etric if and only if A x l = F A 0l A + B + F A A la 0 A + B + F B 0l + CC 0l + C l C 0 A + F CA 0l + CA 0 + CB 0 A + F C 0lA F A 0C l + F C lb 0 + CB 0l A 8 F A + B A + B + C 0 F A Al + B l A + B A + B + A F CA la 0 A Al + B l A l + B l A F B x l + CC xl A A + B C F B xla F C xla A + B. 6. Thus, we have the following results Theore 6.. Let F = A + B + C be a Randers change of generalized th root Finsler etric on a anifold M n. Then, F is a locally dually flat etric if and only if equation 6. satisfied. Corollary 6.. 9. Let F = A be an th root Finsler etric on an open subset U R n. Then F is a locally dually flat etric if and only if the following holds A x l = A A 0A y l + AA 0l. 6.5 Putting C = 0 in equation. and equation 6., we get the following corollary.

78 MANOJ KUMAR Corollary 6.3. 8. Let F = A be an th root Finsler etric on an open subset U R n. Then F = F + B is a locally dually flat etric if and only if the following holds A x l = A 0l + A A la 0 + B 0lA Bx la A + B F. Acknowledgeent: The author expresses his sincere thanks to the Governent of India, DAE Departent of Atoic Energy, Mubai for funding as NBHM National Board for Higher Matheatics Post Doctoral Fellow, which reference nuber is /08/05/R & D-II/909, dated July 08, 05. References P.L. Antonelli, R. Ingarden, M. Matsuoto, The Theory of Sprays and Finsler Spaces with Applications in Physics and Biology, Kluwer Acadeic, Dordrecht, 993. V. Balan, N. Brinzei, Berwald-Moor-type h, v-etric physical odels, Hypercoplex Nubers in Geoetry and Physics, 005, no.,. 3 B. Li, Z. Shen, On projectively flat fourth root etrics, Canad. Math. Bull. 55 0 38 5. M. Matsuoto, On Finsler spaces with Randers etric and special fors of iportant tensors, J. Math. Kyoto Univ. 97 77 98. 5 M. Matsuoto, H. Shiada, On Finsler spaces with -for etric. II. Berwald Moor s etric L = y y... y n /n, Tensor N.S. 3 978 75 78. 6 G. Randers, On an asyetric etric in the four-space of general relativity, Phys. Rev. 59 9 95 99. 7 H. Shiada, On Finsler spaces with the etric L = a i... y i....y i, Tensor N.S. 33 979 365 37. 8 A. Tayebi, On generalized th root etrics of isotropic scalar curvature, Math. Slovaca 68 08 907 98. 9 A. Tayebi, B. Najafi, On -th root Finsler etrics, J. Geo. Phys. 6 0 79 8. 0 A. Tayebi, E. Peyghan, M. Shahbazi Nia, On generalized -th root Finsler etrics, Linear Algebra Appl. 37 0 675 683. B. Tiwari, G.Kr. Prajapati, On Einstein Kropina change of -th root Finsler etrics, Differ. Geo. Dyn. Syst. 8 06 39 6. B. Tiwari, M. Kuar, On Randers change of a Finsler space with -th root etric, Int. J. Geo. Methods Modern Phys. 0, no. 0, 50087, 3 pp. 3 Y. Yu, Y. You, On Einstein -th root etrics, Differential Geo. Appl. 8 00 90 9. DST-Centre for Interdisciplinary Matheatical Sciences, Institute of Science, Banaras Hindu University, Varanasi-005, India. E-ail address: veraath@gail.co