• Nie Znaleziono Wyników

The natural operators lifting vector fields to the bundle of affinors

N/A
N/A
Protected

Academic year: 2021

Share "The natural operators lifting vector fields to the bundle of affinors"

Copied!
6
0
0

Pełen tekst

(1)

U N I V E R S I T A T I S M A R I A E C U R I E - S K Ł O D O W S K A L U B L I N – P O L O N I A

VOL. LXII, 2008 SECTIO A 75–80

JAN KUREK and WŁODZIMIERZ M. MIKULSKI

The natural operators lifting vector fields to the bundle of affinors

Abstract. All natural operators T T (T ⊗ T) lifting vector fields X from n-dimensional manifolds M to vector fields B(X) on the bundle of affinors T M ⊗ TM are described.

1. Introduction. In [3], the second author studied the problem how a 1- form ω on an n-manifold M induces a 1-form B(ω) on T M ⊗ TM . This problem was reflected in natural operators B : T T(T ⊗ T) over n- manifolds. It is proved that the set of natural operators T T(T ⊗ T) over n-manifolds is a free C(Rn)-module of dimension 2n, and there is presented a basis of this module.

In this note we study a similar problem how a vector field X on an n- manifold M induces a vector field B(X) on T M ⊗ TM . This problem is reflected in natural operators T T (T ⊗ T) over n-manifolds. We prove that the set of natural operators T T (T ⊗ T) over n-manifolds is a free C(Rn)-module of dimension n + 1. We construct a basis of this module.

We recall that a natural operator B : T T (T ⊗ T) over n-manifolds is an Mfn-invariant family of regular operators

B : X (M ) → X (T M ⊗ TM )

2000 Mathematics Subject Classification. 58A20, 53A55.

Key words and phrases. Natural bundles, natural operators.

(2)

for all n-manifolds M . The invariance means that if vector fields X1 on M and X2 on N are ϕ-related for some local diffeomorphism ϕ : M → N between n-manifolds then the vector fields B(X1) and B(X2) are T ϕ ⊗ Tϕ- related. The regularity means that B transforms smoothly parametrized families of vector fields into smoothly parametrized families of vector fields.

From now on x1, . . . , xn are the usual coordinates on Rn and ∂i = ∂xi

for i = 1, . . . , n are the canonical vector fields on Rn. All manifolds and maps are assumed to be of class C. 2. Examples of natural operators T T (T ⊗ T).

Example 2.1. Let X be a vector field on an n-manifold M . Let T ⊗ TX be the flow lifting of X to T M ⊗ TM . More precisely, if ϕt is the flow of X, then T ϕt⊗ Tϕt is the flow of T ⊗ TX. The correspondence T ⊗ T : T T (T ⊗ T) given by X → T ⊗ TX is a natural operator (called the flow operator) in question.

Example 2.2. For k = 0, . . . , n − 1 we have the canonical vector field Lk on T M ⊗ TM such that

Lk(A) = d dt

0

(A + tAk), A ∈ End(TxM ) = TxM ⊗ TxM, x ∈ M, where Akis the k-th power of A (A0= id). The vector field Lkwill be called the k-th Liouville vector field on T M ⊗ TM (L1 is the classical Liouville vector field on T M ⊗ TM ). The correspondence Lk: T T (T ⊗ T) is a natural operator in question.

3. The C(Rn)-module of natural operators T T (T ⊗ T) over n-manifolds. If L : V → V is an endomorphism of an n-dimensional vector space V then a1(L), . . . , an(L) denote the coefficient of the characteristic polynomial

WL(λ) = det(λidV − L) = λn+ a1(L)λn−1+ · · · + an−1(L)λ + an(L).

Thus for every n-manifold M we have maps a1, . . . , an: T M ⊗ TM → R (as TxM ⊗ TxM = End(TxM )).

The vector space of all natural operators B : T T (T ⊗ T) over n- manifolds is additionally a module over the algebra C(Rn) of smooth maps Rn → R. Actually given a smooth map f : Rn → R and a natural operator B : T T (T ⊗ T) we have natural operator f B : T T (T ⊗ T) given by

(f B)(X) = f (a1, . . . , an)B(X) for any vector field X on an n-manifold M .

(3)

4. The main result. The main result of this short note is the following classification theorem.

Theorem 1. The flow operator T ⊗ T together with the k-th Liouville operators Lk for k = 0, . . . , n − 1 form a basis of the C(Rn)-module of natural operators T T (T ⊗ T) over n-manifolds.

The proof of Theorem 1 will occupy the rest of this note.

5. The result of J. Dębecki. The vector space End(Rn) of all endo- morphisms of Rnis a GL(n)-space because of the usual (adjoint) action of GL(n) on End(Rn).

We have the following result of J. Dębecki.

Proposition 1 ([1]). Any GL(n)-equivariant map C : End(Rn) → End(Rn) is of the form

C(A) =

n−1

X

k=0

fk(a1(A), . . . , an(A))Ak for some uniquely determined maps fk: Rn→ R.

6. The vertical type natural operators B : T T (T ⊗ T) over n-manifolds. A natural operator B : T T (T ⊗ T) is of vertical type if B(X) is a vertical vector field for any vector field X on a n-manifold.

Using Proposition 1 we prove the following fact.

Proposition 2. The C(Rn)-submodule of vertical type natural operators B : T T (T ⊗ T) over n-manifolds is free and n-dimensional. The k-th Liouville operators Lk for k = 0, . . . , n − 1 form a basis of this module.

Proof. Let B : T T (T ⊗ T) be a vertical type natural operator over n-manifolds. Because of the naturality and the Frobenius theorem this operator is uniquely determined by the restriction of vertical vector field B(∂1) to the fiber End(T0Rn) = T0Rn× T0Rn.

Using the naturality of B with respect to the homotheties tidRn for t 6= 0 we see that

B(∂1)|End(T0Rn)= B(t∂1)|End(T0Rn)

for t 6= 0. Putting t → 0 we see that

B(∂1)|End(T0Rn)= B(0)|End(T0Rn).

Because of the naturality of B(0) with respect to linear automorphisms of Rn we have a GL(n)-equivariant map

C : End(T0Rn) → End(T0Rn)

(4)

given by

B(0)(A) = d dt

0

(A + tC(A)) for A ∈ End(T0Rn).

By Proposition 1 we have that C(A) =

n−1

X

k=0

fk(a1(A), . . . , an(A))Ak for some uniquely determined maps fk: Rn→ R. Then

B(∂1)(A) =

n−1

X

k=0

fk(a1(A), . . . , an(A))Lk(A) for all A ∈ End(T0Rn). That is why B =Pn−1

k=0fkLk, as well.  7. Proof of Theorem 1. It is clear that Theorem 1 will be proved after proving the following fact.

Proposition 3. Let B : T T (T ⊗ T) be a natural operator over n- manifolds. Then there exists a unique map f : Rn→ R such that B − f T ⊗ T is a vertical type operator.

Let π : T Rn⊗ TRn→ Rn be the bundle projection.

Lemma 1. There exist unique maps fk ∈ C(Rn) such that T π(B(wo)(A)) =

n−1

X

k=0

fk(a1(A), . . . , an(A))Ak(w)

for A ∈ End(T0Rn) = T0Rn⊗ T0Rn and w ∈ T0Rn, where wo is the

“constant” vector field on Rn with wo0= w.

Proof. By the invariance of B with respect to the homotheties tidRn for t 6= 0 we have the homogeneity condition

T π(B((tw)o)(A) = tT π(B(wo))(A).

Then by the homogeneous function theorem, [2], T π(B(wo)(A) depends linearly on w.

So, we can define a map C : End(T0Rn) → End(T0Rn) by C(A)(w) = T π(B(wo)(A))

for all A ∈ End(T0Rn) and w ∈ T0Rn.

Because of the naturality of B with respect to linear automorphisms of Rn, C is GL(n)-equivariant. Then applying Proposition 1 we end the

proof. 

Lemma 2. Let B : T T (T ⊗ T) be as in Lemma 1. Let f0, . . . , fn−1 be the maps from Lemma 1. Then fj = 0 for j = 1, . . . , n − 1.

(5)

Proof. Consider j = 1, . . . , n − 1. Let b = (b1, . . . , bn) ∈ Rn. Let A ∈ End(T0Rn) be such that A(∂i(0)) = ∂i+1(0) for i = 1, . . . , n − 1 and A(∂n(0)) = −bn1(0) − . . . − b1n(0). Then ai(A) = bi for i = 1, . . . , n.

Let ϕt= (x1, . . . , xj+1+txj+1+. . . , . . . , xn) be the flow of ∂j+1+xj+1j+1 near 0 ∈ Rn.

Since T0ϕ1◦ A ◦ T0ϕ−11 6= A (as the left hand side evaluated at ∂j(0) is equal to 2∂j+1(0) and the right hand side evaluated in the same vector ∂j(0) is equal to ∂j+1(0)), we have

(1) T ⊗ T(xj+1j+1)(A) 6= 0.

Using the Zajtz theorem [4], since (∂j+1+ xj+1j+1)(0) = ∂j+1(0) 6= 0, we find a diffeomorphism η : R → R such that

(2) j10ψ = id

and

(3) ψj+1= ∂j+1+ xj+1j+1

near 0 ∈ Rn, where ψ(x1, . . . , xn) = (x1, . . . , xj, η(xj+1), . . . , xn).

Clearly ψ preserves ∂1. Because of (2), ψ preserves A. Then ψ preserves B(∂1)(A).

Because of (2), ψ preserves any vertical vector tangent to T Rn⊗ TRn at A. Moreover, ψ preserves all ∂l for l = 1, . . . , n with l 6= j + 1. By (3), ψ sends T ⊗ T(∂j+1)(A) into T ⊗ T(∂j+1+ xj+1j+1)(A). Then ψ sends B(∂1)(A) =

n−1

X

k=0

fk(a1(A), . . . , an(A))T ⊗T(∂k+1)(A)+some vertical vector into B(∂1)(A) + fj(b)T ⊗ T(xj+1j+1)(A).

Then because of (1), we have fj(b) = 0, as well.  Proof of Proposition 3. Because of Lemmas 1 and 2 we have

B(∂1)(A) = f0(a1(A), . . . , an(A))T ⊗ T(∂1)(A) + some vertical vector for any A ∈ End(T0Rn). Since B is determined by B(∂1) over 0, the proof

of Proposition 3 is complete. 

References

[1] Dębecki, J., Natural transformations of affinors into functions and affinors, Suppl.

Rend. Circolo Mat. Palermo 30(II) (1993), 101–112.

[2] Kol´r, I., Michor, P. W. and Slov´ak, J., Natural Operations in Differential Geometry, Springer-Verlag, Berlin, 1993.

[3] Mikulski, W. M., Liftings of 1-forms to the bundle of affinors, Ann. Univ. Mariae Curie-Skłodowska Sect. A 65 (2001), 109–113.

[4] Zajtz, A., On the order of natural differential operators and liftings, Ann. Polon. Math.

49 (1988), 169–175.

(6)

Jan Kurek Włodzimierz M. Mikulski Institute of Mathematics Institute of Mathematics Maria Curie-Skłodowska University Jagiellonian University pl. Marii Curie-Skłodowskiej 1 ul. Łojasiewicza 6

20-031 Lublin, Poland 30-348 Kraków, Poland

e-mail: kurek@hektor.umcs.lublin.pl e-mail: mikulski@im.uj.edu.pl Received January 4, 2008

Cytaty

Powiązane dokumenty

We discuss the open problem of analytic hypoellipticity for sums of squares of vector fields, including some recent partial results and a conjecture of Treves.. The well known

The purpose of this paper is to develop the theory of Markov operators acting on the space M E of vector measures defined on Borel subsets of a compact metric space X.. These

Furthermore, in this case, the maximum number of periodic orbits that bifurcate from infinity inside the family and for small perturbations is i − 1.. (c) The maximum number of

For such vector fields, we get an estimate of energy from below which, in the case of spheres S n , n > 3, appears to be sharp and is attained by (and only by) totally geodesic

The regularity of A means that A transforms smoothly parametrized families of pairs of trivializations of P and torsion free classical linear connections on M into smoothly

The problem has been considered only for local vector fields and the full and positive answer is known whenever X has a nonvanishing germ.. From now on the notation X(R n ) will be

2. We will state Bott’s theorem in a general form, after intro- ducing the concept of an equivariant sheaf, which is a useful extension of the original defi- nition given in [B2].

4.. fibered surjective submersions between fibered manifolds) and in a paper being in preparation they extend Kol´ aˇ r’s result [7] to product- preserving bundle functors on F 2