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2 1 The proof

n n+p n Let f : M → Qc˜ be an isometric immersion of a Riemannian manifold M n+p into the space form Qc˜ . If the immersion f has flat normal bundle, that is, if at any point the curvature tensor of the normal connection vanishes, then it is a standard fact (cf. [7]) that at any point x ∈ M n there exists a set of unique pairwise distinct normal vectors ηi(x) ∈ Nf M(x), 1 ≤ i ≤ s(x), called the principal normals of f at x, and an associate orthogonal splitting of the as

TxM = Eη1 (x) ⊕···⊕ Eηs (x), where

Eηi (x)= X ∈ TxM : αf (X,Y )= hX,Y iηi for all Y ∈ TxM .  n The multiplicity of a principal normal ηi ∈ Nf M(x) of f at x ∈ M is the dimension of the tangent subspace Eηi (x). If s(x) = k is constant on n n M , then the maps x ∈ M 7→ ηi(x), 1 ≤ i ≤ k, are smooth vector fields, called the principal normal vector fields of f. Moreover, also the distributions n x ∈ M 7→ Eηi (x), 1 ≤ i ≤ k, are smooth. n n+p In the sequel, let f : Mc → Qc˜ , c< c˜, be an isometric immersion with flat normal bundle. Since C =˜c − c> 0, it follows from the Gauss equation that any principal normal has multiplicity one. Thus, there exist exactly n nonzero principal normal vector fields η1,...,ηn satisfying

hηi, ηji = C, 1 ≤ i =6 j ≤ n. (1)

If Xi ∈ Γ(Eηi ), 1 ≤ i ≤ n, is a unit local vector field then the local orthonor- mal frame X1,...,Xn diagonalizes the second fundamental form of f, that is, αf (Xi,Xj)= δijηi, 1 ≤ i, j ≤ n, where δij is the Kronecker delta. Such a frame is called a principal frame. Lemma 3. The following holds:

∇Xi Xj = −λiXj(1/λi)Xi, 1 ≤ i =6 j ≤ n, (2)

2 where λi =1 kηik + C. p 3 Proof: The Codazzi equation is equivalent to

⊥ ∇Xj ηi = h∇Xi Xi,Xji(ηi − ηj) (3) and

h∇Xℓ Xj,Xii(ηi − ηj)= h∇Xj Xℓ,Xii(ηi − ηℓ) (4) for all 1 ≤ i =6 j =6 ℓ =6 i ≤ n. The vectors ηi − ηj and ηi − ηℓ, 1 ≤ i =6 j =6 ℓ =6 i ≤ n are linearly independent. Suppose otherwise that ηi − ηj = µ(ηi − ηℓ). Taking the inner 2 product with ηi and using (1) gives kηik = C < 0, a contradiction. It now follows from (4) that

i j ∇Xi Xj =ΓijXi +ΓijXj, i =6 j,

k j where Γij = h∇Xi Xj,Xki. Since Γij = h∇Xi Xj,Xji = 0, then

i j ∇Xi Xj =ΓijXi = −ΓiiXi.

On the other hand, taking the inner product of (3) with ηi and using (1) is j easily seen to give that Γii = λiXj(1/λi), as we wished.

n Lemma 4. For each x0 ∈ Mc there exists a diffeomorphism F : U → V from n an open subset U ⊂ R endowed with coordinates {u1,...,un} onto an open n neigborhood V ⊂ Mc of x0 such that the tangent frame

2 2 kη1k + CF∗(∂/∂u1),..., kηnk + CF∗(∂/∂un) (5) p p n is orthonormal and principal. Moreover, if Mc is complete and simply con- n n nected then F : R → Mc is a diffeomorphism. Proof: For the local existence, observe that Lemma 3 implies

[λiXi,λjXj]=0, 1 ≤ i =6 j ≤ n.

For the proof of the global part, we follow a similar argument as in the n proof of Theorem 3 in [9] or Proposition 5.6 in [7]. Assume that Mc is n complete and simply connected. Set Yi = λiXi and let ϕi(x, t), x ∈ Mc , t ∈ R be the one-parameter group of diffeomorphisms generated by Yi. Since the vector fields Yi, 1 ≤ i ≤ n, have bounded lengths, it follows that ϕi(x, t) is n defined for all values of x and t. Thus, for any x ∈ Mc , the map t 7→ ϕi(x, t)

4 n is the integral curve of Yi with ϕi(x, 0) = x. Let x0 be a fixed point in Mc n n and define a function F = Fx0 : R → Mc by

F (t1, t2,...,tn)= ϕn(ϕn−1(··· ϕ2(ϕ1(x0, t1), t2), ··· ), tn).

Since the Lie bracket [Yi,Yj] vanishes the parameter groups ϕi and ϕj com- mute. This implies that

F (t + s)= ϕ (ϕ − (··· ϕ (ϕ (F (s), t ), t ), ··· ), t )= F (t) (6) x0 n n 1 2 1 x0 1 2 n Fx0 (s) where t =(t1,...,tn) and s =(s1,...,sn). Thus d d F∗(s)∂ = | F (s ,...,s + t,...,s )= | ϕ (F (s), t)= Y (F (s)). i dt t=0 1 i n dt t=0 i i n We claim that F is a covering map. Then this and that Mc is simply connected yields that F is a diffeomorphism, which gives the proof. n ˜ Given x ∈ Mc , let B2ε(0) be an open ball of radius 2ε centered at the ˜ origin such that Fx|B˜2ε(0) is a diffeomorphism onto B2ε(x)= Fx(B2ε(0)). Set −1 {x˜α}α∈A = F (x) and denote by B˜2ε(˜xα) the open ball of radius 2ε centered atx ˜α. Define a map φα : B2ε(x) → B˜2ε(˜xα) by −1 φα(y)=˜xα + Fx (y). From (6) we obtain F (φ (y)) = F (˜x + F −1(y)) = F (F −1(y)) = F (F −1(y)) = y x0 α x0 α x Fx0 (˜xα) x x x ˜ for all y ∈ B2ε(x). Thus Fx0 is a diffeomorphism from B2ε(˜xα) onto B2ε(x) having φα as its inverse. In particular, this implies that B˜2ε(˜xα) and B˜2ε(˜xβ) are disjoint if α, β ∈ A are distinct indices. Finally, it remains to check that −1 ˜ ify ˜ ∈ Fx0 (Bε(x)), theny ˜ ∈ Bε(˜xα) for some α ∈ A. This follows from the fact that F (˜y − F −1(F (˜y))) = F (−F −1(F (˜y))) = x. x0 x x0 Fx0 (˜y) x x0 n For the last equality, observe from (6) that for all x, y ∈ Mc we have Fx(t)= y if and only if Fy(−t)= x. n The third fundamental form IIIf (x) of f at x ∈ M is given by

IIIf (X,Y )(x)=tr hαf (X, · ),αf (Y, · )i,X,Y ∈ TxM.

Since αf has no kernel (that is, positive index of relative nullity), then IIIf (x) is a positive definite inner product.

5 0 Lemma 5. The Riemannian metric g = Cg + IIIf is flat where g is the n 0 metric of Mc . Moreover, the metric g is complete if g is complete.

Proof: In terms of the system of principal coordinates {u1,...,un} given by Lemma 4, we have

2 0 C kηik gij = Cgij + IIIf (∂/∂ui,∂/∂uj )= 2 δij + 2 δij = δij. kηik + C kηik + C

0 0 Moreover, the metric g is complete since gij >Cgij.

n n Proof of Theorem 1. By Nikolayevsky’s result we have that Mc = Hc . Let n n F : R → Hc be the global diffeomorphism given by Lemma 4. We endow Rn with the pullbacks of the two metrics considered in Lemma 5 that are still denoted by g and g0. Notice that (Rn, g0) is the standard flat . Given a smooth curve γ :[a, b] ⊂ R → Rn set

2 Sˆ(γ) = max kαf k (F (γ(t))). t∈[a,b]

We have from (5) that 1 1 gij = 2 δij ≥ δij. kηik + C Sˆ(γ)+ C Then, the lengths of γ satisfy

1/2 Lg0 (γ) < (Sˆ(γ)+ C) Lg(γ). (7)

Let γ :[a, b] → Rn andγ ˜ :[a, b] → Rn be the unique Euclidean and hyperbolic geodesics, respectively, joining γ(a)=˜γ(a) to γ(b)=˜γ(b). From (7) we have ˆ 1/2 Lg0 (γ) ≤ Lg0 (˜γ) < (S(˜γ)+ C) Lg(˜γ). n Thus, if γx,y is the unique hyperbolic geodesic joining x =6 y ∈ R , then the distances with respect to g0 and g satisfy

ˆ 1/2 dg0 (x, y) < (S(γx,y)+ C) dg(x, y). (8)

n g g0 Fix x0 ∈ R and let Dr (x0) and Dr (x0) be the closed geodesic balls of 0 radius r> 0 centered at x0 with respect to g and g , respectively.

6 It holds that g g0 Dr (x0) ⊂ int D (x0) , (9)  ψ(r)  where ψ(r)= r(S(r)+ C)1/2 and S(r) = max (kα k2(F (x))). g f x∈Dr (x0)

g In fact, if y ∈ Dr (x0) we have using (8) that 1/2 1/2 0 ˆ ˆ dg (x0,y) < (S(γx0,y)+ C) dg(x0,y) ≤ r(S(γx0,y)+ C) ≤ ψ(r). Then, we obtain using (9) that the volumes of the geodesic balls satisfy

g g0 Volg(Dr (x0)) ≤ Volg Dψ(r)(x0)  n 2 −1/2 = Πi=1(kηik + C) du1 ∧···∧ dun Z g0 Dψ(r)(x0)

−n/2 −n/2 g0 < C du ∧···∧ du = C Vol 0 D (x ) 0 1 n g ψ(r) 0 ZDg (x ) ψ(r) 0  n n/2 = r (1 + S(r)/C) ωn,

g where ωn is the volume of the Euclidean unit n-ball. Since Volg(Dr (x0)) is well known to grow exponentially with r (for instance, see [5]), it follows that also S(r) grows exponentially with r, and thus the second fundamental form of f has exponential growth. Remark 6. It is worth mentioning that it was shown in [6] that there is no isometric immersion with flat normal bundle of a complete Riemannian n n+p manifold Mc , c > 0, into Qc˜ with c < c˜. Notice that this follows using Lemma 4.

References

[1] Aminov, Y., Extrinsic geometric properties of the Rozendorn surface, which is an isometric immersion of the Lobachevski plane into E5. Sb. Math. 200 (2009), 1575–1586. [2] Bolotov, D., On an isometric immersion with a flat normal connection of the Lobachevsky space Ln into the Euclidean space Rn+m, Math. Notes 82 (2007), 10–12.

7 [3] Brander, D., Results related to generalizations of Hilbert’s non- immersibility theorem for the hyperbolic plane, Electron. Res. Announc. Math. Sci. 15 (2008), 8–16.

[4] Cartan, E., Sur les vari´et´es de courbure constante d’un espace euclidien ou non-euclidien, Bull. Soc. Math. France 47 (1919), 125–160; 48 (1920), 132–208.

[5] Chavel, I., “Riemannian Geometry: A Modern Introduction” Cambridge University Press, Cambridge, 1993.

[6] Dajczer M. and Tojeiro, R., Isometric immersions and the generalized Laplace and elliptic sinh-Gordon equations, J. Reine Angew. Math. 467 (1995), 109–147.

[7] Dajczer M. and Tojeiro, R., “Submanifold theory beyond an introduc- tion”. Universitext. Springer, 2019.

[8] Gromov, M., Geometric, algebraic, and analytic descendants of Nash isometric embedding theorems, Bull. Amer. Math. Soc. 54 (2017), 173– 245.

[9] Moore, J. D., Isometric immersions of space forms in space forms, Pacific J. Math. 40 (1972), 157–166.

[10] Moore, J. D., Problems in the geometry of submanifolds, Mat. Fiz. Anal. Geom. 9 (2002),648–662,

[11] Y. Nikolayevsky, Non-immersion theorem for a class of hyperbolic man- ifolds, Differential Geom. Appl. 9 (1998) 239–242.

[12] Yau, S.-T., Seminar on Differential Geometry, Ann. of Math. Stud. 102, Princeton Univ. Press, Princeton, N.J. (1982), 669–706,

Marcos Dajczer IMPA – Estrada Dona Castorina, 110 22460–320, Rio de Janeiro – Brazil e-mail: [email protected]

Christos-Raent Onti Department of Mathematics and Statistics

8 University of Cyprus 1678, Nicosia – Cyprus

Theodoros Vlachos University of Ioannina Department of Mathematics Ioannina – Greece e-mail: [email protected]

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