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Parallel transport on non-collapsed 𝖱𝖢𝖣(𝐾, 𝑁) spaces

  • Emanuele Caputo , Nicola Gigli EMAIL logo and Enrico Pasqualetto ORCID logo
Published/Copyright: December 13, 2024

Abstract

We provide a general theory for parallel transport on non-collapsed RCD spaces obtaining both existence and uniqueness results. Our theory covers the case of geodesics and, more generally, of curves obtained via the flow of sufficiently regular time dependent vector fields: the price that we pay for this generality is that we cannot study parallel transport along a single such curve, but only along almost all of these (in a sense related to the notions of Sobolev vector calculus and regular Lagrangian flow in the non-smooth setting). The class of ncRCD spaces contains finite-dimensional Alexandrov spaces with curvature bounded from below; thus our construction provides a way of speaking about parallel transport in this latter setting alternative to the one proposed by Petrunin in [Parallel transportation for Alexandrov space with curvature bounded below, Geom. Funct. Anal. 8 (1998), 1, 123–148]. The precise relation between the two approaches is yet to be understood.

Award Identifier / Grant number: 314789

Funding statement: The third named author acknowledges the support by the Academy of Finland (project number 314789) and by the Balzan project led by Luigi Ambrosio.

A Existence of the parallel transport in W 1 , 2 ( π )

In this section, we show an existence result of the parallel transport of an initial vector field along a Lipschitz test plan in the class W 1 , 2 ( π ) . In particular, we can show, by an abstract argument of functional analysis, that, for a given initial vector field V ̄ e 0 L 2 ( T X ) , we can find a Borel vector field t V t along a Lipschitz test plan 𝝅 such that V W 1 , 2 ( π ) , ( D π V ) t = 0 for a.e. 𝑡, and it satisfies the initial condition in an appropriate sense. We use in this section a vanishing viscosity approach: we approximate our problem with a sequence of problems that are coercive; on this class of problems, we can apply a variant of the Lax–Milgram lemma; thanks to compactness, we can pass to the limit and obtain a solution to our problem. More precisely, the variant of the Lax–Milgram lemma is the following, and it is taken from [5].

Lemma A.1

Lemma A.1 (Lions)

Let 𝐸 and 𝐻 be a normed and a Hilbert space respectively. Assume that 𝐸 is continuously embedded in 𝐻, with v H v E for every v E . Let B : H × E R be a bilinear form such that B ( , v ) is continuous for every v E . If 𝐵 is coercive, namely there exists c > 0 such that B ( v , v ) c v E 2 for every v E , then for all l E , there exists h H such that B ( h , v ) = l ( v ) for every v E and

h H l V c .

We introduce the following class of approximations. For a given 𝜀, we solve in a distributional sense the partial differential equation

( D π V ) t = ε ( V t + ( D π 2 V ) t ) ,

looking for a solution in H 1 , 2 ( π ) .

Definition A.2

Definition A.2 (Parallel transport in W 1 , 2 ( π ) )

Let ( X , d , m ) be an RCD ( K , ) space and 𝝅 a Lipschitz test plan on X . Given V ̄ e 0 L 2 ( T X ) , we say that V W 1 , 2 ( π ) is a parallel transport in W 1 , 2 ( π ) of V ̄ along 𝝅 if D π V = 0 and, for every Z TestVF ( π ) ,

(A.1) R ( Z ) 0 = V ̄ , Z 0 d π ,

where we denote by t R ( Z ) t the absolutely continuous representative of t V t , Z t d π .

Theorem A.3

Theorem A.3 (Existence of PT in W 1 , 2 ( π ) )

Let ( X , d , m ) be an RCD ( K , ) space and 𝝅 a Lipschitz test plan on X . Let V ̄ e 0 L 2 ( T X ) be given. Then there exists V W 1 , 2 ( π ) that is a parallel transport in W 1 , 2 ( π ) of V ̄ along 𝝅.

Proof

Fix ε ( 0 , 1 / 2 ) . Consider the Hilbert space H : = ( H 1 , 2 ( π ) , H 1 , 2 ( π ) ) . Define also

E := { Z TestVF ( π ) spt ( Z ) [ 0 , 1 ) } H 1 , 2 ( π ) , Z E := ( Z 0 e 0 L 2 ( T X ) 2 + Z H 2 ) 1 / 2 for every Z E .

Clearly, Z H Z E for every Z E . Now let us define B : H × E R and : E R as

B ( V , Z ) := 0 1 V t , D π Z t + ε V t , Z t + ε D π V t , D π Z t d π d t , ( Z ) := V ̄ , Z 0 d π ,

respectively. The map 𝐵 is bilinear by construction. Moreover, for some constant C > 0 , we have that | B ( V , Z ) | C V H Z H for every V H and Z E ; thus, in particular, B ( , Z ) is continuous for any Z E . The Leibniz rule grants that

2 0 1 Z t , D π Z t d π d t = | Z 0 | 2 d π

holds for every Z E , whence coercivity of the map 𝐵 follows: given any Z E , we have

B ( Z , Z ) = 1 2 | Z 0 | 2 d π + ε 0 1 | Z t | 2 + | D π Z t | 2 d π d t ε Z E 2 .

Furthermore, it holds that E and E V ̄ e 0 L 2 ( T X ) . Therefore, Lemma A.1 yields the existence of an element V ε H such that V ε H V ̄ e 0 L 2 ( T X ) / ε and B ( V ε , Z ) = ( Z ) for every Z E , which explicitly reads as

(A.2) 0 1 V t ε , D π Z t + ε V t ε , Z t + ε D π V t ε , D π Z t d π d t = V ̄ , Z 0 d π

for every Z E . Given any Z TestVF ( π ) and φ LIP ( [ 0 , 1 ] ) with spt ( φ ) [ 0 , 1 ) , it holds that t φ ( t ) Z t belongs to 𝐸 and D π ( φ Z ) t = φ ( t ) Z t + φ ( t ) D π Z t for a.e. t [ 0 , 1 ] . Then

(A.3) φ ( 0 ) V ̄ , Z 0 d π = 0 1 φ ( t ) V t ε , D π Z t + ε V t ε , Z t + ε D π V t ε , D π Z t d π d t + 0 1 φ ( t ) V t ε , Z t + ε D π V t ε , Z t d π d t .

Fix a Lebesgue point s ( 0 , 1 ) of t V t ε , Z t + ε D π V t ε , Z t d π . Define φ n as

φ n ( t ) : = { 1 if t [ 0 , s ) , n ( t s ) + 1 if t [ s , s + 1 / n ) , 0 if t [ s + 1 / n , 1 ] ,

for all n N , n > 1 / ( 1 s ) . Note that ( φ n ) n LIP ( [ 0 , 1 ] ) is a bounded sequence in L ( 0 , 1 ) , spt ( φ n ) [ 0 , 1 ) for all 𝑛, and φ n χ [ 0 , s ] pointwise as n . Moreover, it holds that

0 1 φ n ( t ) V t ε , Z t + ε D π V t ε , Z t d π d t = n s s + 1 / n V t ε , Z t ε D π V t ε , Z t d π d t V s ε , Z s ε D π V s ε , Z s d π as n .

Therefore, by plugging φ = φ n into (A.3) and letting n , we deduce that

(A.4) V ̄ , Z 0 d π = 0 s V t ε , D π Z t + ε V t ε , Z t + ε D π V t ε , D π Z t d π d t + V s ε , Z s ε D π V s ε , Z s d π .

Given that V ε H 1 , 2 ( π ) , we can find a sequence ( Z n ) n TestVF ( π ) that W 1 , 2 ( π ) -converges to V ε . We start noting that, from [24, Theorem 3.23], there exists a continuous injection i : H 1 , 2 ( π ) C ( π ) such that V ε Z n C ( π ) 2 V ε Z n W 1 , 2 ( π ) , which grants that lim n V 0 ε Z 0 n e 0 L 2 ( T X ) = 0 . Therefore, it follows that

lim n V ̄ , Z 0 n d π = V ̄ , V 0 ε d π .

By plugging Z = Z n into (A.4), letting n , and using the Leibniz rule in H 1 , 2 ( π ) , we get

V ̄ , V 0 ε d π = 0 s V t ε , D π V t ε + ε | V t ε | 2 + ε | D π V t ε | 2 d π d t + | V s ε | 2 ε D π V s ε , V s ε d π 0 s V t ε , D π V t ε d π d t + | V s ε | 2 ε D π V s ε , V s ε d π = 1 2 | V s ε | 2 d π + 1 2 | V 0 ε | 2 d π + | V s ε | 2 ε D π V s ε , V s ε d π = 1 2 | V s ε | 2 d π + 1 2 | V 0 ε | 2 d π ε D π V s ε , V s ε d π .

Since 1 2 | V 0 ε | 2 d π V ̄ , V 0 ε d π = 1 2 | V ̄ V 0 ε | 2 d π 1 2 | V ̄ | 2 d π , we can rewrite the former expression as

1 2 | V ̄ V 0 ε | 2 d π 1 2 | V ̄ | 2 d π ε D π V s ε , V s ε d π 1 2 | V s ε | 2 d π .

Therefore, we obtain that

1 2 | V s ε | 2 d π 1 2 | V s ε | 2 d π + 1 2 | V ̄ V 0 ε | 2 d π 1 2 | V ̄ | 2 d π + ε D π V s ε , V s ε d π .

By integrating the above inequality over the interval [ 0 , 1 ] , multiplying by 2, and then applying Young’s inequality a b ε a 2 + b 2 / ( 4 ε ) , we infer that

0 1 | V s ε | 2 d π d s | V ̄ | 2 d π + 2 ε 0 1 D π V s ε , V s ε d π d s | V ̄ | 2 d π + 2 ε 2 0 1 | D π V s ε | 2 d π d s + 1 2 0 1 | V s ε | 2 d π d s ,

whence accordingly

1 2 0 1 | V s ε | 2 d π d s | V ̄ | 2 d π + 2 ε 2 0 1 | D π V s ε | 2 d π d s 3 V ̄ e 0 L 2 ( T X ) 2 .

Observe also that { ε V ε } ε ( 0 , 1 / 2 ) is bounded in 𝐻. Therefore, there exist V L 2 ( π ) , W H , and a sequence ε n 0 such that V ε n V weakly in L 2 ( π ) and ε n V ε n W weakly in 𝐻. In particular, it must hold that W = 0 . Hence, by letting n in the identity

0 1 V t ε n , D π Z t + ε n V t ε n , Z t + D π ( ε n V ε n ) t , D π Z t d π d t = V ̄ , Z 0 d π ,

which holds for every n N and Z TestVF c ( π ) by (A.2), we can finally conclude that

0 1 V t , D π Z t d π d t = 0

is satisfied for every Z TestVF c ( π ) . This grants that V W 1 , 2 ( π ) and D π V = 0 . Finally, let us prove (A.1). Fix any Z TestVF ( π ) and denote by t R ( Z ) t the absolutely continuous representative of t V t , Z t d π (that belongs to W 1 , 1 ( 0 , 1 ) ). Write (A.4) with ε = ε n , integrate over s [ 0 , 1 ] , and then let n : by exploiting the weak convergence V ε n V in L 2 ( π ) (and by using the dominated convergence theorem), we obtain that

V ̄ , Z 0 d π = 0 1 0 s V t , D π Z t d π d t d s + 0 1 V s , Z s d π d s = 0 1 0 s ( d d t R ( Z ) t ) d t d s + 0 1 R ( Z ) s d s = 0 1 R ( Z ) s R ( Z ) 0 d s + 0 1 R ( Z ) s d s = R ( Z ) 0 ,

where we applied the Leibniz rule with one vector field in H 1 , 2 ( π ) and the other in W 1 , 2 ( π ) . Hence the statement is achieved. ∎

Acknowledgements

The second named author thanks Prof. G. R. Mingione for some interesting conversations on topics relevant for this work.

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Received: 2022-12-20
Revised: 2024-09-12
Published Online: 2024-12-13
Published in Print: 2025-02-01

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