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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. LVI, 6 SECTIO A 2002

WŁODZIMIERZ M. MIKULSKI

The natural affinors on dual

r

-jet prolongations of bundles of 2-forms

Abstract. Let Jr2T)M be the r-jet prolongation of Λ2TM of an n- dimensional manifold M . For natural numbers r and n ≥ 3 all natural affinors on (Jr2T)M )are the constant multiples of the identity affinor only.

0. Let us recall the following definitions (see e.g. [4]).

Let F : Mfn → F M be a functor from the category Mfn of all n- dimensional manifolds and their local diffeomorphisms into the category F M of fibered manifolds. Let B be the base functor from the category of fibered manifolds to the category of manifolds.

A natural bundle over n-manifolds is a functor F satisfying B ◦F = id and the localization condition: for every inclusion of an open subset iU : U → M , F U is the restriction p−1M (U ) of pM : F M → M over U and F iU is the inclusion p−1M(U ) → F M .

An affinor Q on a manifold M is a tensor type (1, 1), i.e. a linear mor- phism Q : T M → T M over idM.

1991 Mathematics Subject Classification. 58A20, 53A55.

Key words and phrases. natural bundles, natural transformations, natural affinors.

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A natural affinor on a natural bundle F is a system of affinors Q : T F M → T F M on F M for every n-manifold M satisfying T F f ◦ Q = Q ◦ T F f for every local diffeomorphism f : M → N .

A connection on a fibre bundle Y is an affinor Γ : T Y → T Y on Y such that Γ ◦ Γ = Γ and im(Γ) = V Y , the vertical bundle of Y .

A natural connection on a natural bundle F is a system of connections Γ : T F M → T F M on F M for every n-manifold M which is (additionally) a natural affinor on F .

In [5] it was shown how natural affinors Q on some natural bundles F M can be used to study the torsion τ = [Γ, Q] of connections Γ on the same bundles F M . That is why natural affinors have been classified in many papers, [1]-[3], [6]-[11].

In this paper one considers the natural bundle F = (Jr2T))which as- sociates to every n-manifold M the vector bundle (Jr2T))M = (Jr2T)M ), where Jr2T)M = {jrxω | ω is a 2-form on M , x ∈ M }, and to every embedding ϕ : M → N of n-manifolds the induced vec- tor bundle mapping (Jr2T))ϕ = (Jr2T−1) : (Jr2T)M ) → (Jr2T)N ), where the map Jr2T)ϕ : Jr2T)M → Jr2T)N is given by jxrω → jrϕ(x)ω).

For integers r ≥ 1 and n ≥ 3 we classify all natural affinors on (Jr2T))M . We prove that every natural affinor Q on (Jr2T))M is proportional to the identity affinor.

We note that the classification of natural affinors on (JrTM )is differ- ent. In [9] we proved that for n ≥ 2 the vector space of all natural affinors on (JrTM ) is 2-dimensional.

The above result shows that ”torsion” of a connection Γ on (Jr2T))M makes no sense because of [Γ, id] = 0.

The above result also shows that for integers r ≥ 1 and n ≥ 3 there are no natural connections on (Jr2T)) over n-manifolds.

The usual coordinates on Rnare denoted by xiand ∂i= ∂xi, i = 1, ..., n.

All manifolds and maps are assumed to be of class C.

1. We start with the classification of all linear natural transformations A : T (Jr2T))M → (Jr2T))M in the sense of [4] over n-manifolds M .

A natural transformation T (Jr2T)) → (Jr2T))over n-manifolds is a system of fibered maps A : T (Jr2T))M → (Jr2T))M over idM

for every n-manifold M satisfying (Jr2T))f ◦ A = A ◦ T (Jr2T))f for every local diffeo. f : M → N . The linearity means that A gives a linear map Ty(Jr2T))M → (Jr2T))xM for any y ∈ (Jr2T))xM , x ∈ M .

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Proposition 1. If n ≥ 3 and r are natural numbers then every linear natural transformation A : T (Jr2T))→ (Jr2T)) over n-manifolds is 0.

Proof. Every element from the fibre (Jr2T))0Rnis a linear combination of the (jr0(xαdxi∧ dxj)) for all α ∈ (N ∪ {0})n with |α| ≤ r and i, j = 1, ..., n, i < j, where the (j0r(xαdxi∧ dxj)) form the basis dual to the j0r(xαdxi∧ dxj) ∈ (Jr2T))0Rn for α and i, j as beside.

Consider a linear natural transformation A : T (Jr2T))→ (Jr2T)) over n-manifolds.

Clearly, A is uniquely determined by the values hA(u), j0r(xαdxi∧dxj)i ∈ R for u ∈ (T (Jr2T))Rn)0=R˜ n×(V (Jr2T))Rn)0=R˜ n×(Jr2T))0 Rn× (Jr2T))0Rn, α ∈ (N ∪ {0})nwith |α| ≤ r and i, j = 1, ..., n, i < j, where ˜= is the standard trivialization and the canonical identification.

Since A is invariant with respect to the coordinate permutations, A is uniquely determined by the values hA(u), jr0(xαdx1∧ dx2)i, where u and α are as above.

If |α| ≥ 1, then the local diffeomorphisms ϕα= (x1, x2, x3+xα, x4, ..., xn)−1 sends j0r(x3dx1∧ dx2) into j0r(x3dx1∧ dx2) + j0r(xαdx1∧ dx2). Then by the invariance of A with respect to the ϕ’s, A is uniquely determined by the values hA(u), j0r(x3dx1∧ dx2)i ∈ R and hA(u), j0r(dx1∧ dx2)i ∈ R, where u ∈ (T (Jr2T))Rn)0=R˜ n× (Jr2T))0Rn× (Jr2T))0Rn.

The proof of Proposition 1 will be complete after proving that hA(u), j0r(dx1 ∧ dx2)i = 0 and hA(u), j0r(x3dx1 ∧ dx2)i = 0 for any u ∈ (T (Jr2T))Rn)0 = R˜ n × (Jr2T))0Rn × (Jr2T))0Rn. We will prove these conditions in Lemmas 1 — 6.

At first we study the values hA(u), j0r(dx1∧ dx2)i.

Lemma 1. There exist the numbers λ, µ, ν ∈ R such that (1) hA(u), j0r(dx1∧ dx2)i = λu11u21+ µu2,(0),1,2+ νu3,(0),1,2

for every u = (u1, u2, u3) ∈ Rn× (Jr2T))0Rn× (Jr2T))0Rn, where u1= (u11, ..., un1) ∈ Rn, uτ,α,i,j is the coefficient of uτ ∈ (Jr2T))0Rn on (j0r(xαdxi∧ dxj)), τ = 2, 3, (0) = (0, ..., 0) ∈ (N ∪ {0})n.

Proof of Lemma 1. By the naturality of A with respect to the homotheties at= (t1x1, ..., tnxn) for t = (t1, ..., tn) ∈ Rn+,

hA(T (Jr2T))(at)(u)), j0r(dx1∧ dx2)i = t1t2hA(u), j0r(dx1∧ dx2)i for any t = (t1, ..., tn) ∈ Rn+. For t ∈ Rn, i, j = 1, ..., n, i < j and α ∈ (N ∪ {0})nwe have T (Jr2T))(at)((j0r(xαdxi∧dxj))) = tα+ei+ej(j0r(xαdxi∧ dxj)). Then the lemma follows from the homogeneous function theorem, [4]. 

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Lemma 2. We have λ = µ = ν = 0.

Proof of Lemma 2. Since hA(u1, u2, u3), j0r(dx1∧dx2)i is linear in (u1, u3) for u2, we have λ = µ = 0. Then (in particular) we have

(2) hA(∂1 |wC ), j0r(dx1∧ dx2)i = hA(e1, w, 0), j0r(dx1∧ dx2)i = 0 for w ∈ (Jr2T))0Rn, where ( )C is the complete lift.

To prove ν = 0 it is sufficient to show that

hA(0, 0, (j0r(dx1∧ dx2))), j0r(dx1∧ dx2)i = 0.

But we have

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0 = hA(((x1)r+11)|wC), j0r(dx1∧ dx2)i

= (r + 1)hA(0, w, (j0r(dx1∧ dx2))+ ... ), j0r(dx1∧ dx2)i

= (r + 1)hA(0, 0, (j0r(dx1∧ dx2))), jr0(dx1∧ dx2)i ,

where w = (j0r((x1)rdx1∧ dx2)) and the dots mean the linear combination of the (j0r(xαdxi∧ dxj)) with (j0r(xαdxi∧ dxj))6= (jr0(dx1∧ dx2)).

Let us explain (3).

Let ϕt be the flow of (x1)r+11. We have h((x1)r+11)|wC , j0r(dx1∧ dx2)i

= hd

dt|t=0(Jr2T))0t)(w), j0r(dx1∧ dx2)i

= d dt|t=0

h(Jr2T))0t)(w), j0r(dx1∧ dx2)i

= d dt|t=0

hw, j0r((ϕ−t)(dx1∧ dx2))i

= hw, j0r( d

dt|t=0−t)(dx1∧ dx2))i

= hw, j0r(L(x1)r+11(dx1∧ dx2))i

= (r + 1)hw, j0r((x1)rdx1∧ dx2)i = r + 1 .

Then ((x1)r+11)C|w = (r + 1)(j0r(dx1 ∧ dx2)) + ... under the canonical isomorphism Vw((Jr2T))Rn) ˜=(Jr2T))0Rn, i.e. hA(((x1)r+11)C|w), j0r(dx1∧ dx2)i = (r + 1)hA(0, w, (j0r(dx1∧ dx2))+ ... ), j0r(dx1∧ dx2)i.

The equality (r + 1)hA(0, w, (jr0(dx1∧ dx2)) + ... ), j0r(dx1∧ dx2)i = (r + 1)hA(0, 0, (jr0(dx1∧ dx2))), j0r(dx1∧ dx2)i is clear because of (1) and µ = 0.

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We can prove the equality 0 = hA(((x1)r+11)|wC ), j0r(dx1∧ dx2)i as fol- lows. Vector fields ∂1+ (x1)r+11and ∂1have the same r-jets at 0. Then by [11], there exists a diffeomorphism ϕ : Rn → Rn such that j0r+1ϕ = id and ϕ1= ∂1+ (x1)r+11near 0. Clearly, ϕ preserves j0r(dx1∧ dx2) because of the jet argument. Then, by the naturality of A with respect to ϕ, it follows from (2) that

hA((∂1+ (x1)r+11)C|w), j0r(dx1∧ dx2)i = 0

for any w ∈ (Jr2T))0Rn. Now, applying the linearity of A, we end the proof of the equality. 

Now, we study the values hA(u), jr0(x3dx1∧ dx2)i = 0.

Lemma 3. There exist the numbers a, b, c, e, f, g ∈ R such that (4) hA(u), j0r(x3dx1∧ dx2)i = au11u2,(0),2,3+ bu21u2,(0),1,3

+ cu31u2,(0),1,2+ eu3,e1,2,3+ f u3,e2,1,3+ gu3,e3,1,2

for any u = (u1, u2, u3), where u1 = (u11, ..., un1) ∈ Rn, u2, u3 ∈ (Jr(T∧ T))0Rn, uτ,α,i,j is as in Lemma 1 and ei= (0, ..., 1, 0, ..., 0) ∈ (N ∪ {0})n, 1 in i-position.

Proof of Lemma 3. The proof is similar to the proof of Lemma 1. We ap- ply the naturality of A with respect to the homotheties at= (t1x1, ..., tnxn) for t = (t1, ..., tn) ∈ Rn+, the homogeneous function theorem and the linear- ity of A. 

To prove g = f = e = a = b = c = 0 we shall use the following Lemma 4. For every u ∈ (T (Jr2T))Rn)0 we have

(5) hA(u), j0r(x3dx1∧ dx2)i = hA(u0), j0r(x3dx1∧ dx2)i , where u0 is the image of u by (x2, x3, x1) × idRn−3.

Proof of Lemma 4. We consider u ∈ (T (Jr2T))Rn)0. Let ˜u be the image of u by (x1+ x1x3, x2, ..., xn). By Lemma 2 we have λ = µ = ν = 0, i.e. hA(˜u), j0r(dx1∧ dx2)i = hA(u), j0r(dx1 ∧ dx2)i = 0. Then by the invariance of A with respect to (x1+ x1x3, x2, ..., xn)−1 we get

0 = hA(u), j0r(dx1∧ dx2)i + hA(u), j0r(x3dx1∧ dx2)i − hA(u), j0r(x1dx2∧ dx3)i as (x1+x1x3, x2, ..., xn)−1sends j0r(dx1∧dx2) into j0r(dx1∧dx2)+j0r(x3dx1∧ dx2) − j0r(x1dx2∧ dx3). Hence hA(u), j0r(x3dx1∧ dx2)i = hA(u), j0r(x1dx2∧ dx3)i. Therefore we have (5) because (x2, x3, x1) × idRn−3 sends j0r(x1dx2∧ dx3) into j0r(x3dx1∧ dx2). 

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Lemma 5. We have g = f = e = 0.

Proof of Lemma 5. We have to show

hA(0, 0, (j0r(x3dx1∧ dx2))), j0r(x3dx1∧ dx2)i

= hA(0, 0, −(j0r(x2dx1∧ dx3))), j0r(x3dx1∧ dx2)i

= hA(0, 0, (j0r(x1dx2∧ dx3))), j0r(x3dx1∧ dx2)i = 0.

We see that (x2, x3, x1)×idRn−3sends (j0r(x3dx1∧dx2))into −(j0r(x2dx1

∧dx3)) and −(j0r(x2dx1∧ dx3)) into (j0r(x1dx2∧ dx3)). Then due to (5) it suffices to verify that hA(0, 0, (j0r(x3dx1∧ dx2))), j0r(x3dx1∧ dx2)i = 0.

But we have

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0 = hA(((x1)r1)C|w), j0r(x3dx1∧ dx2)i

= rhA(0, w, (j0r(x3dx1∧ dx2))), j0r(x3dx1∧ dx2)i

= rhA(0, 0, (j0r(x3dx1∧ dx2))), j0r(x3dx1∧ dx2)i , where w = (j0r(x3(x1)r−1dx1∧ dx2))∈ (Jr2T))0Rn.

Let us explain (6).

That hA(0, w, (j0r(x3dx1∧ dx2))), j0r(x3dx1∧ dx2)i = hA(0, 0, (j0r(x3dx1

∧dx2))), j0r(x3dx1∧ dx2)i is clear, see (4).

We can prove 0 = hA(((x1)r1)C|w), j0r(x3dx1∧ dx2)i as follows. Vector fields ∂1+ (x1)r1 and ∂1have the same r−1-jets at 0. Then by [11] there exists a diffeomorphism ϕ = ϕ1 × idRn−1 : Rn = R × Rn−1 → Rn = R × Rn−1 such that ϕ1 : R → R, j0rϕ = id and ϕ1 = ∂1+ (x1)r1

near 0. Let ϕ−1 send w into ˜w. Then ˜w is the linear combination of the (j0r(xαdxi∧dxj))∈ (Jr2T))0Rnfor |α| ≥ 1 and i, j = 1, ..., n with i < j.

(For, h ˜w, j0r(dxi∧ dxj)i = hw, j0r(d(xi◦ ϕ−1) ∧ d(xj ◦ ϕ−1))i = 0.) Then, by (4), hA(∂1 | ˜C w), j0r(x3dx1 ∧ dx2)i = hA(e1, ˜w, 0), j0r(x3dx1∧ dx2)i = 0.

Clearly, ϕ preserves j0r(x3dx1∧ dx2). Then, using the naturality of A with respect to ϕ we get hA((∂1+ (x1)r1)C|w), j0r(x3dx1 ∧ dx2)i = 0. Now, applying the linearity of A, we end the proof of equality.

Using the flow argument one can prove hA(((x1)r1)C|w), j0r(x3dx1∧dx2)i=

rhA(0, w, (j0r(x3dx1 ∧ dx2))), j0r(x3dx1 ∧ dx2)i as follows. For any α ∈ (N ∪ {0})n with |α| ≤ r and any i, j = 1, ..., n with i < j we have

h((x1)r1)C|w, j0r(xαdxi∧ dxj)i = hw, j0r(L(x1)r1xαdxi∧ dxj)i

= hw, α1j0r((x1)r−1xαdxi∧ dxj)i + hw, j0r(xαδi1r(x1)r−1dx1∧ dxj)i . Since w = (j0r(x3(x1)r−1dx1∧ dx2)), the sum is equal to r if α = e3 and (i, j) = (1, 2) and equal to 0 in the other cases. Hence ((x1)r1)C|w = r(j0r(x3dx1∧ dx2))∈ Vw(Jr2T))Rn. This ends the proof of hA(((x1)r

1)C|w), j0r(x3dx1∧dx2)i = rhA(0, w, (j0r(x3dx1∧dx2))), j0r(x3dx1∧dx2)i. 

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Lemma 6. We have a = b = c = 0.

Proof of Lemma 6. By (5), similarly as for e = f = g = 0, it is sufficient to prove that c = 0, i.e. hA(∂3 |(jC r0(dx1∧dx2))), j0r(x3dx1∧ dx2)i = 0. But we have

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0 = hA(∂C3 |(j0r((x1)rdx1∧dx2))), j0r(x3dx1∧ dx2)i

= hA(∂C3 |(jr

0(dx1∧dx2))+...), j0r(x3dx1∧ dx2)i

= hA(∂C3 |(j0r(dx1∧dx2))), j0r(x3dx1∧ dx2)i ,

where the dots denote the linear combination of the (j0r(xαdxi∧ dxj)) 6=

(j0r(dx1∧ dx2)) for |α| ≤ r and i, j = 1, ..., n, i < j.

Let us explain (7).

The equality 0 = hA(∂3 |(jC r

0((x1)rdx1∧dx2))), jr0(x3dx1∧ dx2)i follows from (4). Similarly, from (4) we obtain hA(∂3 |(jC 0r(dx1∧dx2))+...), j0r(x3dx1∧dx2)i=

hA(∂3 |(jC r

0(dx1∧dx2))), j0r(x3dx1∧ dx2)i.

We consider the local diffeomorphism ϕ = (x1+r+11 (x1)r+1, x2, ..., xn)−1. We see that ϕ−1 preserves j0r(x3dx1∧ dx2) and ∂3. Moreover, we see that ϕ−1sends (j0r((x1)rdx1∧dx2))into (j0r(dx1∧dx2))+..., where the dots are as above, because of h(j0r((x1)rdx1∧ dx2)), j0r(dx1∧ dx2))i = 1. Now, by the invariance of A with respect to ϕ−1we get hA(∂3 |(jC r0((x1)rdx1∧dx2))), j0r(x3dx1∧ dx2)i = hA(∂3 |(jC 0r(dx1∧dx2))+...), j0r(x3dx1∧ dx2)i. 

The proof of Proposition 1 is complete. 

2. The tangent map T π : T (Jr2T))M → T M of the bundle pro- jection π : (Jr2T))M → M defines a linear natural transformation T π : T (Jr2T))→ T over n-manifolds. (The definition of linear natural transformations T (Jr2T)) → T over n-manifolds is similar to the one of Section 1.)

Proposition 2. If r and n ≥ 2 are natural numbers, then every linear natu- ral transformation B : T (Jr2T))→ T over n-manifolds is proportional to T π.

Proof. Due to similar arguments as in the proof of Proposition 1, B is uniquely determined by the values hB(u), d0x1i for u ∈ (T (Jr2T))Rn)0

˜

=Rn× (Jr2T))0Rn× (Jr2T))0Rn.

By the naturality of B with respect to the homotheties (t1x1, ..., tnxn) for t ∈ Rn+and the homogeneous function theorem we deduce that hB(.), dx1i = x1◦ p1, where p1 : Rn × (Jr2T))0Rn × (Jr2T))0Rn → Rn is the canonical projection.

Then the vector space of all B as above is 1-dimensional. 

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3. The main result of this paper is the following theorem.

Theorem 1. If n ≥ 3 and r are natural numbers, then every natural affinor Q on (Jr2T)) over n-manifolds is a constant multiple of id.

Proof. Let Q : T (Jr2T))M → T (Jr2T))M be a natural affinor on (Jr2T)) over n-manifolds. Then B = T π ◦ Q : T (Jr2T))→ T is a linear natural transformation. By Proposition 2, B = T π ◦ Q = λT π for some λ. Clearly, T π ◦ id = T π. Then Q − λid is an affinor of vertical type.

Now, applying Proposition 1 we deduce that Q − λid is the zero affinor.  From Theorem 1 we obtain immediately

Corollary 1. If n ≥ 3 and r are natural numbers, then there is no natural connection on (Jr2T)) over n-manifolds.

References

[1] Doupovec, M., Natural transformations between T T TM and T TT M , Czech Math.

J. 43(118) (1993), 599–613.

[2] Doupovec, M., I. Kol´r, Natural affinors on time-dependent Weil bundles, Arch.

Math. (Brno) 27 (1991), 205–209.

[3] Gancarzewicz, J., I. Kol´r, Natural affinors on the extended r-th order tangent bun- dles, Suppl. Rendiconti Circolo Mat. Palermo 30 (1993), 95–100.

[4] Kol´r I., P.W. Michor and J. Slov´ak, Natural operations in differential geometry, Springer-Verlag, Berlin, 1993.

[5] Kol´r, I., M. Modugno, Torsions of connections on some natural bundles, Diff.

Geom. and Appl. 2 (1992), 1–16.

[6] Kurek, J., Natural affinors on higher order cotangent bundles, Arch. Math. (Brno) 28 (1992), 175–180.

[7] Mikulski, W.M., Natural affinors on r-jet prolongation of the tangent bundle, Arch.

Math. (Brno) 34(2) (1998), 321–328.

[8] Mikulski, W.M., The natural affinors on ⊗kT(r), Note di Matematica 19(2) (1999), 269–274.

[9] Mikulski, W.M., The natural affinors on (JrT), Arch. Math. (Brno) 36(4) (2000), 261–267.

[10] Mikulski, W.M., The natural affinors on generalized higher order tangent bundles, Rend. Mat. Roma 21(VII) (2001), 339–349.

[11] Zajtz, A., On the order of natural operators and liftings, Ann. Polon. Math. 49 (1988), 169–178.

Institute of Mathematics received February 7, 2001 Jagiellonian University

Krak´ow, Reymonta 4, Poland e-mail: mikulski@im.uj.edu.pl

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