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Başlık: Semi-parallel tensor product surfaces in semi-euclidean space E42Yazar(lar):YILDIRIM, Mehmet; ILARSLAN, KazımCilt: 65 Sayı: 2 Sayfa: 133-141 DOI: 10.1501/Commua1_0000000765 Yayın Tarihi: 2016 PDF

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D O I: 1 0 .1 5 0 1 / C o m m u a 1 _ 0 0 0 0 0 0 0 7 6 5 IS S N 1 3 0 3 –5 9 9 1

SEMI-PARALLEL TENSOR PRODUCT SURFACES IN

SEMI-EUCLIDEAN SPACE E4

2

MEHMET YILDIRIM AND KAZIM ·ILARSLAN

Abstract. In this article, the tensor product surfaces are studied that arise from taking the tensor product of a unit circle centered at the origin in

Euclid-ean plane E2and a non-null, unit planar curve in Lorentzian plane E2

1. Also we

have shown that the tensor product surfaces in 4-dimensional semi-Euclidean space with index 2; E4

2;satisfying the semi-parallelity condition R(X; Y ):h = 0

if and only if the tensor product surface is a totally geodesic surface in E4

2:

1. Introduction

B. Y. Chen initiated the study of the tensor product immersion of two im-mersions of a given Riemannian manifold [6]. This concept originated from the investigation of the quadratic representation of submanifold. Inspired by Chen’s de…nition, F. Decruyenaere, F. Dillen, L. Verstraelen and L. Vrancken studied in [8] the tensor product of two immersions of, in general, di¤erent manifolds. Under some conditions, this realizes an immersion of the product manifold.

Let M and N be two di¤erentiable manifolds and assume that f : M ! Em;

and

g : N ! En

are two immersions. Then the direct sum and tensor product maps are de…ned respectively by f h : M N ! Em+n (p; q) ! f(p) h(q) = (f1(p); : : : ; fm(p); h1(q); : : : ; hn(q)) and f h : M N ! Emn (p; q) ! f(p) h(q) = (f1(p)h1(q); : : : ; f1(p)hn(q); : : : ; fm(p)hn(q))

Received by the editors: March 18, 2016, Accepted: May 14, 2016.

2010 Mathematics Subject Classi…cation. Primary 53C40; Secondary 53C15.

Key words and phrases. Tensor product immersion, Euclidean circle, Lorentzian curves, semi-parallel surface, normal curvature.

c 2 0 1 6 A n ka ra U n ive rsity C o m m u n ic a tio n s d e la Fa c u lté d e s S c ie n c e s d e l’U n ive rs ité d ’A n ka ra . S é rie s A 1 . M a th e m a t ic s a n d S t a tis tic s .

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Necessary and su¢ cient conditions for f h to be an immersion were obtained in [7]. It is also proved there that the pairing ( ; ) determines a structure of a semiring on the set of classes of di¤erentiable manifolds transversally immersed in Euclidean spaces, modulo orthogonal transformations. Some semirings were studied in [8]. In the special case, a tensor product surface is obtained by taking the tensor product of two curves. In many papers, minimality and totally reality properties of a tensor product surfaces were studied for example [2], [10], [11], [12]. The relations between a tensor product surface and a Lie group was shown in [15], [16]. In [2], Bulca and Arslan studied tensor product surfaces in 4- dimensional Euclidean space E4and they show that tensor product surfaces satisfying the semi-parallelity condition R(X; Y ):h = 0 are totally umbilical surface.

In this article, we investigate a tensor product surface M which is obtained from two curves. One of them is a unit circle centered at the origin in Euclidean plane E2 and a non-null, unit planar curve in Lorentzian plane E21. Firstly, we investigated some geometric properties of the tensor product surface in pseudo-Euclidean 4-space E4

2 then we obtain the su¢ cient and necessary conditions for the surface satisfying the semi parallelity condition R(X; Y ):h = 0:

We remark that the notions related with pseudo- Riemannian geometry are taken from [14].

2. Preliminaries

In the present section we give some de…nitons about Riemannian submanifolds from [5] and [4]. Let : M ! En be an immersion from an m dimensional connected Riemannian manifold M into an n dimensional Euclidean space En . We denote by g the metric tensor of En as well as induced metric on M . Let r be the Levi- Civita connection of En and r the induced connection on M. Then the Gaussian and Weingarten formulas are given by

rXY = rXY + h(X; Y )

(2.1) rXN = ANX + r?XN

where X; Y are vector …elds tangent to M and N is normal to M . Moreover, h is the second fundamental form, r?is linear connection induced in the normal bundle T?M , called normal connection and AN is the shape operator in the direction of N that is related with h by

< h(X; Y ); N >=< ANX; Y > : (2.2) If the set fX1; ::; Xmg is a local basis for (M) and fN1; :::; Nn mg is an orthonor-mal local basis for ?(M ); then h can be written as

h = n mP =1 m P i;j=1 hijN ; (2.3)

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where

hij =< h(Xi; Xj); N > :

The covariant di¤erentiation rh of the second fundamental form h on the direct sum of the tangent bundle and the normal bundle T M T?M of M is de…ned by (rXh)(Y; Z) = r?Xh(Y; Z) h(rXY; Z) h(Y; rXZ); (2.4) for any vector …elds X; Y and Z tangent to M . Then we have the Codazzi equation as

(rXh)(Y; Z) = (rYh)(X; Z): (2.5)

We denote by R the curvature tensor associated with r;

R(X; Y )Z = rXrYZ + rYrXZ + r[X;Y ]Z; (2.6) and denote by R? the curvature tensor associated with r?

R?(X; Y ) = r?Yr?X r?Xr?Y r?[X;Y ] : (2.7) The equations Gauss and Ricci are given by

< R(X; Y )Z; W >=< h(X; W ); h(Y; Z) > < h(X; Z); h(Y; W ) >; (2.8) < R(X; Y ) ; > < R?(X; Y ) ; >=< [A ; A ]X; Y >; (2.9) for any vector …elds X; Y; Z,W tangent to M and ; normal vector …elds to M .

The Gaussian curvature of M is de…ned by

K =< h(X1; X1); h(X2; X2) > kh(X1; X2)k2 (2.10) where the set fX1; X2g is a linearly independent subset of (M):

The normal curvature KN of M is de…ned by KN = 8 < : n 2X 1= < < R?(X1; X2)N ; N >2 9 = ; 1=2 (2.11) where fN ; N g is an orthonormal basis of ?(M ): From (2.11) we conclude that KN = 0 if and only if r? is a ‡at normal connection of M .

Further, the mean curvature vectorH of M is de…ned by! ! H = 1 m n mX =1 tr(AN )N (2.12)

Let us consider the product tensor R:h of the curvature tensor R with the second fundamental form h is de…ned by

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for all X; Y; Z; T tangent to M:

The surface M is said to be semi - parallel (or semi-symmetric ) if R:h = 0, i.e. R(X; Y ):h = 0 [9], [17]. It is easily seen that

(R(X; Y ):h)(Z; T ) = R?(X; Y )h(Z; T ) h(R(X; Y )Z; T ) h(Z; R(X; Y )T ) (2.14) Lemma 2.1. [9] Let M En be a smooth surface given with the patch X(u,v). Then the following equalities are hold;

(R(X1; X2):h)(X1; X1) = n 2P =1 h11(h22 h11+ 2K) h(X1; X2) + n 2P =1 h11h12(h(X1; X1) h(X2; X2)) (R(X1; X2):h)(X1; X2) = n 2P =1 h12(h22 h11) h(X1; X2) + n 2P =1 h12h12 K (h(X1; X1) h(X2; X2)) (R(X1; X2):h)(X2; X2) = n 2P =1 h22(h22 h11 2K) h(X1; X2) + n 2P =1 h22h12(h(X1; X1) h(X2; X2)) 9 > > > > > > > > > > > > > > > > > > = > > > > > > > > > > > > > > > > > > ; (2.15) Semi parallel surfaces classi…ed by J. Deprez [9].

Theorem 2.1. [9]Let M be a surface in n- dimensional Euclidean space En: Then M is semi-parallel if and only if locally;

i) M is aquivalent to 2-sphere, or ii)M has trivial normal connection, or

iii) M is an isotropic surface in E5 En satisfying kHk2 = 3K:

3. Tensor product surfaces of a Euclidean plane curve and a Lorentzian plane curve

Minimal and pseudo-minimal tensor product surfaces of a Lorentzian plane curve and a Euclidean plane curve was studied by I. Mihai and et al. in [13]. They also gave some examples of non-minimal pseudo-umbilical tensor product surfaces. It is well konown that the tensor product of two immersions is not commutative.Thus the tensor product surfaces of a Euclidean plane curve and a Lorentzian plane curve is a new surface in 4-dimensional semi-Euclidean space with index 2.

In the following section, we will consider the tensor product immersions which is obtained from a Euclidean plane curve and a Lorentzian plane curve. Let c1 : R !E2be a Euclidean plane curve and c

2: R !E21 be a non-null Lorentzian plane curve. Put c1(t) = ( 1(t); 2(t)) and c2(s) = ( 1(s); 2(s)):

Then their tensor product surface is given by x = c1 c2: R2! E42

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x(t; s) = ( 1(t) 1(s); 1(t) 2(s); 2(t) 1(s); 2(t) 2(s)): The metric tensor on E2

1 and E42is given by g = dx21+ dx22 and

g= dx21+ dx22 dx23+ dx24; respectively.

If we take c1 as a Euclidean unit circle c1(t) = (cos t; sin t) at centered origin and c2(s) = ( (s); (s)) is a spacelike or timelike curve with unit speed then the surface patch becomes

M : x(t; s) = ( (s) cos t; (s) cos t; (s) sin t; (s) sin t) (3.1) An orthonormal frame tangent to M is given by

e1 = 1 kc2k @x @t = 1 kc2k

( (s) sin t; (s) sin t; (s) cos t; (s) cos t);

(3.2) e2 =

@x @s

= ( 0(s) cos t; 0(s) cos t; 0(s) sin t; 0(s) sin t): The normal space of M is spanned by

n1 = (

0

(s) cos t; 0(s) cos t; 0(s) sin t; 0(s) sin t); (3.3) n2 =

1 kc2k

( (s) sin t; (s) sin t; (s) cos t; (s) cos t) where g(e1; e1) = g(n2; n2) = g(c2(s); c2(s)) kc2k2 = "1; (3.4) g(e2; e2) = g(n1; n1) = g(c 0 2(s); c 0 2(s)) = "2 and "1= 1; "2= 1:

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By covariant di¤erentiation with respect to e1and e2 a straightforward calcula-tion gives re1e1= a"2e2 b"2n1 re1e2= a"1e1 b"1n2 re1n1= b"1e1 a"1n2 re1n2= b"2e2+ a"2n1 (3.5) re2e1= b"1n2 re2e2= c"2n1 re2n1= c"2e2 re2n2= b"1e1 (3.6)

where a, b and c are Christo¤el symbols and as in follows a = a(s) = 0 0 kc2k2 ; (3.7) b = b(s) = 0 0 kc2k2 ; (3.8) c = c(s) = 0 00 00 0: (3.9)

In addition, from (2.3) second fundamental form of this structure is written as, h = 2 P i;j; =1 " hijn ; (3.10) where h111= b h211= 0 h112= h121= 0 h212= h221= b h1 22= c h222= 0 (3.11) By considering equations (3.8) and 3.9, we conclude that

Corollary 3.1. If b = 0 then c is also zero: Also by using Corollary 3.1 and (3.11), we have Corollary 3.2. M is a totally geodesic surface in E4

2 if and only if b = 0 which means that c2 is a straightline passing through the origin.

If b = 0, from (3.8), we get c2(s) = (s)( ; 1). Since M is a non-degenerate surface, the position vector of c2 cannot be a null then 6= 1. In this case, we can write the parametric equation of tensor product surface M as follows

M : x(t; s) = ( (s) cos t; (s) cos t; (s) sin t; (s) sin t); 6= 1; 2 R. Indeed, this surface fully lies in a cone surface passing through the origin (but not light cone) in 4-dimensional semi-Euclidean space with index 2, E4

2; with equation x2 1+ 2 x2 2 x23+ 2 x2 4= 0 where 6= 1 and 2 R.

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The induced covariant di¤erentiation on M as in follows, re1e1 = a"2e2; re1e2 = a"1e1; re2e1 = 0; re2e2 = 0: 9 > > = > > ; (3.12) r?e1n1 = a"2n2; r?e1n2 = a"2n1; 9 = ; (3.13) r?e2n1 = 0; r?e2n2 = 0 (3.14) where the equalities (3.13) and (3.14) de…ne the normal connection on M . Lemma 3.1. Let x = c1 c2 be a tensor product immersion of a Euclidean unit circle c1 at centered origin and unit speed non-null Lorentzian curve c2 in E21 . Then the shape operators of M in direction of n1 and n2 are given by respectively,

An1 =

b"1 0

0 c"2 ; An2=

0 b"1

b"2 0 . (3.15)

By a simple calculation, we see that Gauss and Ricci equations of M are identical and they are given by as follow

a0 a2"1= b2"1 bc"2; (3.16) and Codazzi equation of M is

b0 = 2ab"1 ac"2: (3.17)

Thus we give the following theorem.

Theorem 3.1. If M is a tensor product surface of a Euclidean unit circle at cen-tered origin and a non-null unit speed Lorentzian curve in E21 then the Christo¤ el symbols of M satisfy the following Riccati equation

(a + b)0= "1(a + b)2 c"2(a + b) : (3.18) Theorem 3.2. Let M be a tensor product surface given with the surface patch (3.1). Then there exist following relation between Gaussian curvature K and normal curvature KN

KN = jKj = b2"1 bc"2

Theorem 3.3. Let M be a tensor product surface given with the surface patch (3.1) . Then the followings are equivalent,

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i) r? is a ‡at connection, ii) KN = K = 0;

iii) b = 0 or "1b = "2c:

Now, we suppose that M is a semi parallel surface, i.e., R:h = 0: From (2.15) we get b2" 1(c b + 2b"1 2c"2) = 0; b"2(b b"1+ c"2)(c b) = 0; b"1(2b2"1+ bc c2 2bc"2) = 0; 9 = ;: (3.19)

Theorem 3.4. Let M be a tensor product surface given with the surface patch (3.1). Then M is a semi parallel surface if and only if

i) For "1= "2, either b = 0 or b = c, ii)For "16= "2, b = 0.

Corollary 3.3. Let M be a tensor product surface given with the surface patch (3.1) with "16= "2 then M is a semi parallel surface if and only if M is a a totally geodesic surface in E4

2.

References

[1] K. Arslan, B. Bulca, B. K¬l¬c, Y. H. Kim , C. Murathan and G. Ozturk, Tensor Product Surfaces with Pointwise 1-Type Gauss Map, Bull. Korean Math.Soc. 48 (2011), 601-609.

[2] K. Arslan and C. Murathan, Tensor product surfaces of pseudo-Euclidean planar curves,

Geometry and topology of submanifolds, VII (Leuven, 1994/Brussels, 1994) World Sci. Publ., River Edge, NJ (1995), 71-74.

[3] B. Bulca and K. Arslan, Semiparallel tensor product surfaces in E4, Int. Electron. J. Geom.,

7,1,(2014), 36-43.

[4] M. do Carmo, Riemannian geometry, Birkhauser, 1993.

[5] B. Y. Chen, Geometry of Submanifolds, M. Dekker, New York 1973.

[6] B. Y. Chen, Di¤erential Geometry of semiring of immersions, I: General Theory Bull. Inst. Math. Acad. Sinica 21 (1993), 1-34.

[7] F. Decruyenaere, F. Dillen, I. Mihai and L. Verstraelen, Tensor products of spherical and equivariant immersions Bull. Belg. Math. Soc.- Simon Stevin 1 (1994), 643-648.

[8] F. Decruyenaere, F. Dillen, L. Verstraelen and L. Vrancken, The semiring of immersions of manifolds, Beitrage Algebra Geom. 34 (1993), 209-215.

[9] J. Deprez, Semi- parallel Surfaces in Euclidean Space, J. Geom., 25 (1985), 192-200.

[10] K. ·Ilarslan and E. Nesovic, Tensor product surfaces of a Lorentzian space curve and a

Lorentzian plane curve, Bull. Inst. Math. Acad. Sinica 33 (2005), 151-171.

[11] K. ·Ilarslan and E. Nesovic, Tensor product surfaces of a Euclidean space curve and a

Lorentzian plane curve, Di¤erential Geometry - Dynamical Systems 9 (2007),47-57. [12] I. Mihai, and B. Rouxel, Tensor Product Surfaces of Euclidean Plane Curves, Results in

Mathematics, 27 (1995), no.3-4, 308-315.

[13] I. Mihai, I. Van de Woestyne, L. Verstraelen and J. Walrave, Tensor product surfaces of a Lorentzian plane curve and a Euclidean plane curve. Rend. Sem. Mat. Messina Ser. II 3(18) (1994/95), 147–158.

[14] B. O‘Neill, Semi - Riemannian Geometry, with applications to relavity, Academic Press. New York, (1983)

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[15] S. Özkald¬ Karaku¸s and Y. Yayli, Bicomplex number and tensor product surfaces in R42,

Ukrainian Math. J. 64 (2012), no. 3, 344–355.

[16] S. Özkaldi and Y. Yayli, Tensor product surfaces in R4 and Lie groups, Bull. Malays. Math.

Sci. Soc. (2) 33 (2010), no. 1, 69–77.

[17] Z. I., Szabo, Structure theorems on Riemannian spaces satisfying R(X; Y )R = 0, I. The local version, J. Di¤erential Geometry, 17 (1982), 531-582.

Current address : M. Y¬ld¬r¬m: K¬r¬kkale University, Faculty of Sciences and Arts, Department of Mathematics, 71450 K¬r¬kkale/ Turkey

E-mail address : myildirim@kku.edu.tr

Current address : K. ·Ilarslan: K¬r¬kkale University, Faculty of Sciences and Arts, Department

of Mathematics, 71450 K¬r¬kkale/ Turkey E-mail address : kilarslan@kku.edu.tr

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