Zum Hauptinhalt springen
Artikel
Lizenziert
Nicht lizenziert Erfordert eine Authentifizierung

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

  • , EMAIL logo und ORCID logo
Veröffentlicht/Copyright: 13. Dezember 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.

References

[1] L. Ambrosio, Transport equation and Cauchy problem for B V vector fields, Invent. Math. 158 (2004), no. 2, 227–260. 10.1007/s00222-004-0367-2Suche in Google Scholar

[2] L. Ambrosio, M. Colombo and S. Di Marino, Sobolev spaces in metric measure spaces: Reflexivity and lower semicontinuity of slope, Variational methods for evolving objects, Adv. Stud. Pure Math. 67, Mathematical Society of Japan, Tokyo (2015), 1–58. 10.2969/aspm/06710001Suche in Google Scholar

[3] L. Ambrosio, N. Gigli and G. Savaré, Calculus and heat flow in metric measure spaces and applications to spaces with Ricci bounds from below, Invent. Math. 195 (2014), no. 2, 289–391. 10.1007/s00222-013-0456-1Suche in Google Scholar

[4] L. Ambrosio, N. Gigli and G. Savaré, Metric measure spaces with Riemannian Ricci curvature bounded from below, Duke Math. J. 163 (2014), no. 7, 1405–1490. 10.1215/00127094-2681605Suche in Google Scholar

[5] L. Ambrosio and D. Trevisan, Well-posedness of Lagrangian flows and continuity equations in metric measure spaces, Anal. PDE 7 (2014), no. 5, 1179–1234. 10.2140/apde.2014.7.1179Suche in Google Scholar

[6] E. Brué, Q. Deng and D. Semola, Improved regularity estimates for Lagrangian flows on RCD ( K , N ) spaces, Nonlinear Anal. 214 (2022), Article ID 112609. 10.1016/j.na.2021.112609Suche in Google Scholar

[7] E. Brué and D. Semola, Constancy of the dimension for RCD ( K , N ) spaces via regularity of Lagrangian flows, Comm. Pure Appl. Math. 73 (2020), no. 6, 1141–1204. 10.1002/cpa.21849Suche in Google Scholar

[8] J. Cheeger, Differentiability of Lipschitz functions on metric measure spaces, Geom. Funct. Anal. 9 (1999), no. 3, 428–517. 10.1007/s000390050094Suche in Google Scholar

[9] J. Cheeger and T. H. Colding, On the structure of spaces with Ricci curvature bounded below. I, J. Differential Geom. 46 (1997), no. 3, 406–480. 10.4310/jdg/1214459974Suche in Google Scholar

[10] J. Cheeger and T. H. Colding, On the structure of spaces with Ricci curvature bounded below. II, J. Differential Geom. 54 (2000), no. 1, 13–35. 10.4310/jdg/1214342145Suche in Google Scholar

[11] J. Cheeger and T. H. Colding, On the structure of spaces with Ricci curvature bounded below. III, J. Differential Geom. 54 (2000), no. 1, 37–74. 10.4310/jdg/1214342146Suche in Google Scholar

[12] T. H. Colding and A. Naber, Sharp Hölder continuity of tangent cones for spaces with a lower Ricci curvature bound and applications, Ann. of Math. (2) 176 (2012), no. 2, 1173–1229. 10.4007/annals.2012.176.2.10Suche in Google Scholar

[13] G. Crippa and C. De Lellis, Estimates and regularity results for the DiPerna–Lions flow, J. Reine Angew. Math. 616 (2008), 15–46. 10.1515/CRELLE.2008.016Suche in Google Scholar

[14] G. De Philippis and N. Gigli, From volume cone to metric cone in the nonsmooth setting, Geom. Funct. Anal. 26 (2016), no. 6, 1526–1587. 10.1007/s00039-016-0391-6Suche in Google Scholar

[15] G. De Philippis and N. Gigli, Non-collapsed spaces with Ricci curvature bounded from below, J. Éc. polytech. Math. 5 (2018), 613–650. 10.5802/jep.80Suche in Google Scholar

[16] R. J. DiPerna and P.-L. Lions, Ordinary differential equations, transport theory and Sobolev spaces, Invent. Math. 98 (1989), no. 3, 511–547. 10.1007/BF01393835Suche in Google Scholar

[17] J. L. Doob, Stochastic processes, Wiley Class. Libr., John Wiley & Sons, New York 1990. Suche in Google Scholar

[18] I. Ganiev and G. S. Mahmuod, The Bochner integral for measurable sections and its properties, Ann. Funct. Anal. 4 (2013), no. 1, 1–10. 10.15352/afa/1399899831Suche in Google Scholar

[19] N. Gigli, Second order analysis on ( P 2 ( M ) , W 2 ) , Mem. Amer. Math. Soc. 1018 (2012), 1–154. Suche in Google Scholar

[20] N. Gigli, On the differential structure of metric measure spaces and applications, Mem. Amer. Math. Soc. 1113 (2015), 1–91. 10.1090/memo/1113Suche in Google Scholar

[21] N. Gigli, Lecture notes on differential calculus on RCD spaces, Publ. Res. Inst. Math. Sci. 54 (2018), no. 4, 855–918. 10.4171/prims/54-4-4Suche in Google Scholar

[22] N. Gigli, Nonsmooth differential geometry—an approach tailored for spaces with Ricci curvature bounded from below, Mem. Amer. Math. Soc. 1196 (2018), 1–161. 10.1090/memo/1196Suche in Google Scholar

[23] N. Gigli and S. Mosconi, The abstract Lewy–Stampacchia inequality and applications, J. Math. Pures Appl. (9) 104 (2015), no. 2, 258–275. 10.1016/j.matpur.2015.02.007Suche in Google Scholar

[24] N. Gigli and E. Pasqualetto, On the notion of parallel transport on RCD spaces, Rev. Mat. Iberoam. 36 (2020), no. 2, 571–609. 10.4171/rmi/1140Suche in Google Scholar

[25] N. Gigli and E. Pasqualetto, Lectures on nonsmooth differential geometry, SISSA Springer Ser. 2, Springer, Cham 2020. 10.1007/978-3-030-38613-9Suche in Google Scholar

[26] N. Gigli and E. Pasqualetto, Equivalence of two different notions of tangent bundle on rectifiable metric measure spaces, Comm. Anal. Geom. 30 (2022), no. 1, 1–51. 10.4310/CAG.2022.v30.n1.a1Suche in Google Scholar

[27] N. Gigli, E. Pasqualetto and E. Soultanis, Differential of metric valued Sobolev maps, J. Funct. Anal. 278 (2020), no. 6, Article ID 108403. 10.1016/j.jfa.2019.108403Suche in Google Scholar

[28] N. Gigli and A. Tyulenev, Korevaar–Schoen’s energy on strongly rectifiable spaces, Calc. Var. Partial Differential Equations 60 (2021), no. 6, Paper No. 235. 10.1007/s00526-021-02028-zSuche in Google Scholar

[29] H. Hahn, Über Annäherung an Lebesgue’sche Integrale durch Riemann’sche Summen, Sitzungsber. Math. Phys. Kl. K. Akad. Wiss. Wien 123 (1914), 713–743. Suche in Google Scholar

[30] P. Hajłasz, Sobolev spaces on an arbitrary metric space, Potential Anal. 5 (1996), no. 4, 403–415. 10.1007/BF00275475Suche in Google Scholar

[31] P. Hajłasz and P. Koskela, Sobolev met Poincaré, Mem. Amer. Math. Soc. 688 (2000), 1–101. 10.1090/memo/0688Suche in Google Scholar

[32] J. Heinonen, Nonsmooth calculus, Bull. Amer. Math. Soc. (N. S.) 44 (2007), no. 2, 163–232. 10.1090/S0273-0979-07-01140-8Suche in Google Scholar

[33] J. Heinonen, P. Koskela, N. Shanmugalingam and J. T. Tyson, Sobolev spaces on metric measure spaces. An approach based on upper gradients, New Math. Monogr. 27, Cambridge University, Cambridge 2015. 10.1017/CBO9781316135914Suche in Google Scholar

[34] R. Henstock, A Riemann-type integral of Lebesgue power, Canad. J. Math. 20 (1968), 79–87. 10.4153/CJM-1968-010-5Suche in Google Scholar

[35] K. Kuwae, Y. Machigashira and T. Shioya, Sobolev spaces, Laplacian, and heat kernel on Alexandrov spaces, Math. Z. 238 (2001), no. 2, 269–316. 10.1007/s002090100252Suche in Google Scholar

[36] J. Lott, An intrinsic parallel transport in Wasserstein space, Proc. Amer. Math. Soc. 145 (2017), no. 12, 5329–5340. 10.1090/proc/13655Suche in Google Scholar

[37] J. Lott and C. Villani, Ricci curvature for metric-measure spaces via optimal transport, Ann. of Math. (2) 169 (2009), no. 3, 903–991. 10.4007/annals.2009.169.903Suche in Google Scholar

[38] M. Muratori and G. Savaré, Gradient flows and evolution variational inequalities in metric spaces. I: Structural properties, J. Funct. Anal. 278 (2020), no. 4, Article ID 108347. 10.1016/j.jfa.2019.108347Suche in Google Scholar

[39] A. Petrunin, Parallel transportation for Alexandrov space with curvature bounded below, Geom. Funct. Anal. 8 (1998), no. 1, 123–148. 10.1007/s000390050050Suche in Google Scholar

[40] A. Petrunin, Alexandrov meets Lott–Villani–Sturm, Münster J. Math. 4 (2011), 53–64. Suche in Google Scholar

[41] T. Rajala, Local Poincaré inequalities from stable curvature conditions on metric spaces, Calc. Var. Partial Differential Equations 44 (2012), no. 3–4, 477–494. 10.1007/s00526-011-0442-7Suche in Google Scholar

[42] G. Savaré, Self-improvement of the Bakry–Émery condition and Wasserstein contraction of the heat flow in RCD ( K , ) metric measure spaces, Discrete Contin. Dyn. Syst. 34 (2014), no. 4, 1641–1661. 10.3934/dcds.2014.34.1641Suche in Google Scholar

[43] K.-T. Sturm, On the geometry of metric measure spaces. I, Acta Math. 196 (2006), no. 1, 65–131. 10.1007/s11511-006-0002-8Suche in Google Scholar

[44] K.-T. Sturm, On the geometry of metric measure spaces. II, Acta Math. 196 (2006), no. 1, 133–177. 10.1007/s11511-006-0003-7Suche in Google Scholar

[45] H.-C. Zhang and X.-P. Zhu, Ricci curvature on Alexandrov spaces and rigidity theorems, Comm. Anal. Geom. 18 (2010), no. 3, 503–553. 10.4310/CAG.2010.v18.n3.a4Suche in Google Scholar

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

© 2024 Walter de Gruyter GmbH, Berlin/Boston

Heruntergeladen am 16.5.2026 von https://www.degruyterbrill.com/document/doi/10.1515/crelle-2024-0082/html?lang=de
Button zum nach oben scrollen