A. MASTROMARTINO and Y. VILLARROEL
LetM be a smoothm-dimensional manifold, and (Ck,nM)0,n ≤m, the man- ifold of co-contact of order k and codimension n over M. Given a differen- tial system (Wk)0 ⊂ (Ck,nM)0 in a neighborhood of X0k ∈ (Wk)0,we asso- ciate with (Wk)0 an ideal Yk(Wk)0 definite in a open of (Ck−1,nM)0. We prove that Yk(Wk)0 is an ideal locally generated by a set of independent 1- forms. It coincides locally with the ideal in Λ∗(Ck−1,nM)0 generated by the setτk−11 ={ω∈Λ1(Ck−1,nM)0/iXω= 0, X ∈τ χk−1(M)}. Here,τ χk−1(M) is the submodule of vector-fields in (Ck−1,nM)0 lying in the distribution that every pointθk−1 of an open in (Ck−1,nM)0 associates with then-dimensionalR-plane Lθk, atθk−1. Moreover, conditions on the differential system (Wk)0 are given for the idealYk(Wk)0 to be a differential closed.
AMS 2000 Subject Classification: Primary 53C15; Secondary 53B25.
Key words: differential system, geometric structure on a manifold, contact theory, co-contact theory.
1. INTRODUCTION
Let M be a smooth m-dimensional manifold, and Ck,nM, n ≤ m, the manifold of contact elements of order kand dimensionnoverM ([4]). Given an n-submanifold S ⊂M, we denote byCxkS a contact element of orderk of S at x ∈S and by ρkr the canonical projection over Cr,nM, with 0 ≤r ≤ k.
Put C0,nM = M. Let TkM ' J0kM be the kth order tangent vector of M, identified with thekth order jet at 0 of curvesγ : (−δ, δ)⊂ < →M,δ≥0 ([1]).
We say that two n-dimensional submanifolds S1, S2 have co-contact of order k and codimension nat x ∈S1∩S2 if the annihilator of the rth order tangent vector at x ∈S1, denoted by (TxrS1)0, coincides with the annihilator of the rth order tangent vector at x∈S2, where 0≤r ≤k([3]).
The equivalence class of co-contact elements of an n-dimensional sub- manifoldS is called the co-contact element of orderkand codimensionnatx, and is denoted by (CxkS)0. The set (Ck,nM)0 of all co-contact elements of or- derkand codimensionnonM has a differentiable manifold structure induced by local bijections with coordinate neighborhoods of the manifold Ck,nM.
REV. ROUMAINE MATH. PURES APPL.,53(2008),2–3, 181–188
By a differential system of order k and dimension n in M we mean an imbedded submanifold W0 ⊂(Ck,nM)0.
One of the result of this paper says that with a system differential (Wk)0 we can associate an ideal Yk(Wk)0 defined in an open (Uk−1)0 of (Wk−1)0= (ρkr)0(Wk)0such that it is an ideal locally generated by (dk−1−n) independent 1-forms, and that there exists a unique distribution τk of dimension n on (Uk−1)0 for which Yk(Wk)0 = Yk−1, the ideal in Λ∗(Ck−1,nM)0 generated by the set τk−11 = {ω ∈ Λ1(Ck−1,nM)0/iXω = 0, X ∈ τ χk−1(M)}, where τ χk−1(M) is the submodule of vector-fields lying inτk.
The first prolongation of ann-submanifoldW0 ⊂(Ck,nM)0 is defined in [3] as
P(W0) = (C1,nW0)0∩(Ck+1,nM)0.
The main result of this paper can be stated as follows. Let W0 ⊂ (Ck,nM)0 be an imbedded submanifold and (Xk)0 ∈ W0. Then Yk(Wk)0 is an ideal differential if and only the map (ρk+1k )0 :P(W0)→W0 is a local submersion in a neighborhood of (Xk)0.
2. CO-CONTACT MANIFOLDS
Given an n dimensional subspace V ⊂TxM, we will denote by V0 the set of forms ω ∈ Tx∗M which annihilate V. We say that two n-dimensional submanifolds S1, S2 have co-contact of order k and codimension n at x ∈ S1 ∩S2 if the annihilator of the rth order tangent vector at x ∈S1, denoted by (TxrS1)0, coincides with the annihilator of the rth order tangent vector at x∈S2, where 0≤r ≤k.
The equivalence class of co-contact elements of an n-dimensional sub- manifold S is called theco-contact element of orderkand codimensionnatx and is denoted by (CxkS)0.
Let us also denote by (Ck,nM)0the set of all co-contact elements of order k and codimensionnoverM, and put (C0,nM)0 =M.
Let (Xk)0 = (CxkS)0 be a co-contact element in (Ck,nM)0, and consider a local coordinate system (V, ϕ = (xi, xj)), 1 ≤ i ≤ n, n+ 1 ≤ j ≤ m, at x∈M, such that {dxi} generates Tx∗S.
Let (V, U, ρ) be a local fibration of V associated with S and let Vk and (Vk)0, the sets of all k-contacts and k-co-contacts of sections of (V, U, ρ), be defined as,
(2.1) Vk=CkV, (Vk)0= (CkV)0. Then the map,
(2.2) ΨkV :Vk→(Vk)0, Cxkg(U)7→(Cxkg(U))0,
is differentiable.
The maps ΨkV allow us to define a differential structure on (Ck,nM)0. A coordinate neighborhood at (Xk)0= (CxkS)0 is given by ((Vk)0, xi, xj, pjI
r), where the{xi, xj, pjI
r}are defined. With this differential structure, the natural injection (ik)0 :S ,→(Ck,nM)0 is given in coordinates as
(ik)0(xi, fj(xi)) =
xi, fj, pjIr(S) = ∂r
∂xi1· · ·∂xir
fj(x)
,
wheref(U) =Sis an imbedding and (ik)0(S), denoted by (CkS)0, is a regular submanifold of dimension n. Moreover, the natural projection
({ωIj
s(xi, fj), 0≤s≤k}) ∈ (Ck,nM)0
y
y(ρkr)0 ({ωjI
s(xi, fj), 0≤s≤r}) ∈ (Cr,nM)0 is a submersion.
Let (Xk)0 = (CxkS)0 be a co-contact element in (Ck,nM)0 and (V, U, ρ) a local fibration of V associated with S atx. Then the diagram,
ΨkV
CkV −→ (CkV)0 ρks
y
y(ρks)0 CsV −→ (CsV)0
ΨsV commutes.
By a differential system of order k and dimension n in M we mean an imbedded submanifoldW0⊂(Ck,nM)0. A solution of a differential systemW0 at (X0k)0 ∈W0 is ann-dimensional imbedded submanifold S⊂M withx0= (ρk0)0((X0k)0)∈S such that (CxkS)0∈W0,x∈S, and (Cxk0S)0 = (X0k)0 ([3]).
A differential systemW0, of orderkand dimensionninM is completely integrableif, given (X0k)0 ∈W0, there exists a solutionS ⊂M at (X0k)0.
3. IDEALS AND MANIFOLD OF CO-CONTACT
If M is a smooth n-dimensional manifold, then we denote by dk the dimension of (Ck,nM)0 and by Fk0(M) the algebra of smooth functions on (Ck,nM)0.
The Lie algebra overRwith respect to the commutator product [X, Y] in the set of all vector-fields on (Ck,nM)0 is denoted by Ξk(M). Let Λi(Ck,nM)0 be the algebra of all smooth i-forms on (Ck,nM)0. The set of all differential
forms on (Ck,nM)0is denoted by Λ?(Ck,nM)0. It has the structure of a module over the ring Fk0 with respect to the operation of wedge product. Let
Tk: (Ck,nM)0 3θk 7→ Tθkk ∈Tθk(Ck,nM)0
be ann-dimensional distribution. Denote byTΞk(M)⊂Ξk(M) the submod- ule of vector fields lying in Tk. Let
Tk1 ={ω ∈Λ1(Ck,nM)0|iXω = 0, X ∈ TΞk(M)},
whereiX is the inner product. Consider the idealYkgenerated in Λ?(Ck,nM)0 by Tk1.
Proposition 3.1. The distribution Tk is integrable if and only if the ideal Yk is a differential closed: dYk⊂ Yk.
Proof. See [7].
Let (Wk)0 ⊂ (Ck,nM)0 be an n-dimensional differential regular sys- tem of order k and (Xk)0 ∈ (Wk)0. We associate with (Wk)0 an ideal de- noted by Y(Wk)0 defined in an arbitrary neighborhood (Uk−1)0 of (Xk−1)0= (ρkk−1)0(Xk)0.
Proposition 3.2. If (ρkk−1)0 is an immersion in a neighborhood (Uk)0 of (Xk)0, then there exists an ideal defined in a open (Uk−1)0 of (Wk−1)0 = (ρkk−1)0(Wk)0, such that it is an ideal locally generated by independent1-forms in (Uk−1)0.
Proof. Let (Wk)0 ⊂ (Ck,nM)0 be a regular differential system and (Xk)0= (CxkS)0 ∈(Wk)0. Let (V, U, ρ) be a local fibration associated withS and (Vk)0 = (CkV)0.
Since (ρkk−1)0 is an immersion in (Uk)0 = (Vk)0 ∩(Wk)0, in the open (Uk−1)0 = (ρkk−1)0(Uk)0 the projection (ρkk−1)0 : (Uk)0 → (Uk−1)0 is a bijec- tion, andσ= (ρkk−1)0−1
|(Uk)0 is a section of the fiber bundle ((Uk)0,(Uk−1)0, (ρkk−1)0).
Now, a point (Yk)0= (Cxkϕ(U))0 ∈(Wk)0∩(Uk)0, whereϕ:U ⊂Rn→ M is an immersion,S =ϕ(U) is identified with the pair (Yk−1)0, L(Yk)0
(see [6]), where (Yk−1)0 =ρkk−1(Yk)0 ∈ (Uk−1)0 while L(Yk)0 ⊂ T(Yk−1)0(Uk−1)0 is the n-dimensional R-plane at (Yk−1)0 corresponding to (Yk)0, i.e.,
(3.1) L(Yk)0 =T(Yk−1)0(ik−1)0(S).
Hence the section σ may be understood as ann-dimensional distribution Tk−1: (Uk−1)0 3(Yk−1)07→Lσ(Yk−1)0.
We can find a local coordinate system (V, xi, xj) and (V0, xi, xj, pjI
k) of x = (ρk0)0(Xk)0 ∈ M and (Xk)0, respectively, such that the section σ is given as σ(xi, xj, pjk−1) while (Wk)0 is represented as
(3.2) pjI
k =FIj
k(xi, xj, pjI
k−1), i= 1, . . . , n, j=n+ 1, . . . , dk−1, with smooth functions FIj
k : (Uk−1)0 →R.
Representation (3.1) shows that Tk−1 is given by the 1-forms (3.3) ωjIr =dpjIr −
n
X
i=1
FIjr−1,idxi, 1≤r≤k, n+ 1≤j ≤dk−1, wheredpjI
0 =dxj andIr,i denotes the orderedr+ 1-uple of integers{1, . . . , n}
given by {i1, . . . , ir, i}.
Hence with (Wk)0 we associated an ideal in Λ?(Ck−1,nM)0, denoted by Y(Wk)0 locally generated by the independent 1-forms ωIj
r in (Uk−1)0. Proposition 3.3.The idealY(Wk)0 coincides locally with the idealYk−1. Proof. Let (Xk)0= (CxkS)0 ∈(Wk)0. Consider the distribution Tk−1 in (Uk−1)0 given by equation (3.2). ThenTk−1 is locally generated by the vector fields in (Uk−1)0 given by
(3.4) (Ck−1S)?
∂
∂xi
x
=Lk−1i =
= ∂
∂xi
(Xk)0 +X
j,Il
pjI
l,i
∂
∂pjI
l
(Xk)0 +X
Ik−1
FIj
k−1,i
∂
∂pjI
k−1
(Xk)0
and the system of 1-forms ωjI
r annihilate the distribution Tk−1 in (Uk−1)0, i.e., a vector field lying in Tk−1 if and only if iXωIj
r = 0, n+ 1 ≤j ≤dk−1. Then the idealY(Wk)0 coincides with the ideal Yk−1 in (Uk−1)0.
The idealY(Wk)0 is called the ideal associated with the differential sys- tem (Wk)0.
The purpose of this paper is to prove
Theorem 3.4. The projection(ρk+1k )0 :P((Wk)0)→ ((Wk)0) is a local submersion on a neighborhood of (Xk)0 ∈((Wk)0) if and only if Yk(Wk)0 is an ideal differential closed.
Proof. Let (Xk)0 ∈ (Wk)0 and ((Vk)0, V,(ρk0)0
(Wk)0 ∩(Vk)0) be the adapted fibration to (Xk)0. Since (Wk)0 ⊂(Ck,nM)0 is a regular n-submani- fold, there are smooth functions
FIi
k : (Vk−1)0 →R
such that (Vk−1)0 is a neighborhood of (ρkk−1)0(Xk)0, and (Wk)0∩(Vk)0 = (xi, xi, FIi
k). Then the idealY(Wk)0 is generated by the set of 1-forms Wj =dxj−
n
X
i=1
pjidxi, WIj
k =dFIj
k−
n
X
i=1
FIj
k,idxi.
Suppose that the projection
(ρk+1k )0:P(Wk)0 →(Wk)0 is a local submersion. Then, given
(Yk)0 = (xi, xi, FIj
k−1, FIj
k)∈(Wk)0∩(Vk)0, there is an element
(Zk)0 = (xi, xj, pjI
k, pjI
k,i)∈P(Wk)0 = (C1,n(Wk)0)0∩(Ck+1,nM)0 such that
(ρk+1k )0(Zk)0 = (Yk)0. Thus,
pjI
k =FIj
k, pjI
k,i= ∂
∂xipjI
k = ∂
∂xiFIj
k
and
pjI
k,i=pjIk−1,α,i =pjIk−1,i,α
in (Wk)0 since (Zk)0 ∈(C1,n(Wk)0)0∩(Ck+1,nM)0.Then, the condition pjI
k−1,α,i(Yk)0=pjI
k−1,i,α(Yk)0
implies that the formal derivatives agree, thus [Li, Lα] = 0, hence wIj
r([Li, Lα]) = 0.
Moreover, dwIj
r(Li, Lα) = 0 for all i, α = 1, . . . , n and 1 ≤ r ≤ k since as wjI
r ∈ Yk(Wk)0 we have dwIj
r(Li, Lα) = LiwIj
r(Lα)−LαwIj
r(Li)− wIj
r([Li, Lα]) = 0.Then dwjI
r ∈ Yk(Wk)0 for all j≥n+ 1, . . . , m, 0≤r ≤k, hence dYk(Wk)0⊂ Yk(Wk)0.
Conversely, suppose now thatdYk(Wk)0 ⊂ Yk(Wk)0. Let (Yk)0∈(Wk)0∩(Vk)0,
where ((Vk)0, V,(ρk0)0) is a local fibration adapted to (Xk)0 ∈ (Wk)0. Then, in coordinates, (Yk)0 = (xi, xj, FIj
k) ∈ (Wk)0 ⊂ (Vk)0), with differentiable functions FIj
k : (Vk−1)0 →R. Let us consider the co-contact element (Zk+1)0 = (xi, xj, pjI
k, pjI
k,i),
where pjI
k = FIj
k. Since dI(Wk)0 ⊂ I(Wk)0, we have [Li, Ls] = 0, where the Li are the fields that spanWck= (Ψk)−1(Wk)0). Therefore,
pjI
k,i=pjI
k−1,α,i =pjI
k−1,i,α. Thus,
(Zk+1)0 ∈(Ck+1,nM)0 since the coordinates
(xi, xj, FIj
k)∈(Wk)0 ⊂(Ck,nM)0.
Furthermore, it is clear that (Zk+1)0 ∈(C1,n(Wk)0)0. Therefore, the projec- tion (ρkk−1)0 :P(Wk)0→(Wk)0 is a local submersion.
Examples 3.5. 1. Let G be the rigid motions group of R3 and H = SO(3). Consider the submanifold (W2)0 ⊂ (C2,2M)0 defined by the section, σ(x1, x2, x3(x1, x2),0,0, k,0,0, k) , i.e., θ3 = 0, $13 =kθ1, $23 = kθ2, k ∈ R, k >0.
Let K ⊂ G be the analytic subgroup of G whose Lie algebra is the annihilator of (W2)0, and let K(0) be the orbit of 0 = π(H), under the restriction ofα toK.
Denote by (Gk)0 the isotropy subgroup of Gof the induced action (αk)0 on the space of co-contact elements at (C0kK(0))0, and by (gk)0 its Lie alge- bra [3].
Then as (W2)0 =G.(C02K(0))0 defines an integrable differential system of order 2 and dimension 2, the ideal Y(W2)0 is differential closed.
2. Consider a homogeneous manifoldM =G/H, a closed subgroupK⊂ G with dimK(0) = n. Let (X2)0 = (C02K(0))0 and assume that G acts transitively on (C1,nM)0.
Let K(z) be a totally geodesic submanifold. By [3], the order of the orbitK(0) is one and, moreover, the orbit K(0) is the solution at (C02K(0))0 of a differential system (W2)0 =G(C02K(0))0 of order 2 and dimension n= dimK(0) overM. Therefore,Y(Wk)0 is an ideal differential closed.
Acknowledgement.This work was supported by CDCHT, Universidad Centro Oc- cidental Lisandro Alvarado, Decanato de Ciencias y Tecnolog´ıas, Barquisimeto, De- partamento de matem´aticas, Barquisimeto, Venezuela.
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Received 15 May 2007 Universidad Centro Occidental Lisandro Alvarado Departamento de matem´aticas
Barquisimeto, Venezuela, amastrom@ucla.edu.ve
and
Universidad Central de Venezuela Escuela de matem´aticas
Caracas, Venezuela yulivilla@yahoo.com