Arnold diffusion

In applied mathematics, Arnold diffusion is the phenomenon of instability of nearly-integrable Hamiltonian systems. The phenomenon is named after Vladimir Arnold who was the first to publish a result in the field in 1964. ^{[1] [2]} More precisely, Arnold diffusion refers to results asserting the existence of solutions to nearly-integrable Hamiltonian systems that exhibit a significant change in the action variables.

Arnold diffusion describes the diffusion of trajectories due to the ergodic theorem in a portion of phase space unbound by any constraints (i.e. unbounded by Lagrangian tori arising from constants of motion) in Hamiltonian systems. It occurs in systems with more than N=2 degrees of freedom, since the N-dimensional invariant tori do not separate the 2N-1 dimensional phase space any more. Thus, an arbitrarily small perturbation may cause a number of trajectories to wander pseudo-randomly through the whole portion of phase space left by the destroyed tori.

Background and statement

For integrable systems, one has the conservation of the action variables. According to the KAM theorem if we perturb an integrable system slightly, then many, though certainly not all, of the solutions of the perturbed system stay close, for all time, to the unperturbed system. In particular, since the action variables were originally conserved, the theorem tells us that there is only a small change in action for many solutions of the perturbed system.

However, as first noted in Arnold's paper, ^[1] there are nearly integrable systems for which there exist solutions that exhibit arbitrarily large growth in the action variables. More precisely, Arnold considered the example of nearly integrable Hamiltonian system with Hamiltonian

${\displaystyle H(I,\phi ,p,q,t)={1 \over 2}I^{2}+{1 \over 2}p^{2}+\epsilon (\cos {q}-1)+\mu (\cos {q}-1)(\sin {\phi +\cos t)}}$

The first three terms of this Hamiltonian describe a rotator-pendulum system. Arnold showed that for this system, for any choice of ${\displaystyle I_{+}>I_{-}>0}$, and for ${\displaystyle 0<\mu \ll \epsilon \ll 1}$, there is a solution to the system for which

${\displaystyle I(0)<I_{-}{\text{ and }}I(T)>I_{+}}$

for some time ${\displaystyle T\gg 0.}$

His proof relies on the existence of 'transition chains' of 'whiskered' tori, that is, sequences of tori with transitive dynamics such that the unstable manifold(whisker) of one of these tori intersects transversally the stable manifold (whisker) of the next one. Arnold conjectured that "the mechanism of 'transition chains' which guarantees that nonstability in our example is also applicable to the general case (for example, to the problem of three bodies)." ^[1]

The KAM theorem and Arnold diffusion has led to a compendium of rigorous mathematical results, with insights from physics. ^{[3] [4]}

General Case

In Arnold's model the perturbation term is of a special type. The general case of Arnold's diffusion problem concerns Hamiltonian systems of one of the forms

(1)${\displaystyle H_{\epsilon }(I,\phi ,p,q)=H_{0}(I,p,q)+\epsilon H_{1}(I,\phi ,p,q,t)}$

where ${\displaystyle (I,\phi ,p,q,t)\in \mathbb {R} ^{m}\times \mathbb {T} ^{m}\times \mathbb {R} ^{n}\times \mathbb {T} ^{n}\times \mathbb {T} ^{1}}$, ${\displaystyle m,n\geq 1}$, and ${\displaystyle H_{0}(I,p,q)}$ describes a rotator-pendulum system, or

(2)${\displaystyle H_{\epsilon }(I,\phi )=H_{0}(I)+\epsilon H_{1}(I,\phi ,t)}$

where ${\displaystyle (I,\phi ,t)\in \mathbb {R} ^{N}\times \mathbb {T} ^{N}\times \mathbb {T} ^{1}}$, ${\displaystyle N\geq 2.}$

For systems as in (1) , the unperturbed Hamiltonian possesses smooth families of invariant tori that have hyperbolic stable and unstable manifolds; such systems are referred to as a priori unstable. For system as in (2) , the phase space of the unperturbed Hamiltonian is foliated by Lagrangian invariant tori; such systems are referred to as a priori stable. ^[5] In either case, the Arnold diffusion problem asserts that, for `generic' systems, there exists ${\displaystyle \rho >0}$ such that for every ${\displaystyle \epsilon >0}$ sufficiently small there exist solution curves for which

${\displaystyle \|I(T)-I(0)\|\geq \rho }$

for some time ${\displaystyle T\gg 0.}$ Precise formulations of possible genericity conditions in the context of a priori unstable and a priori stable system can be found in, ^{[6] [7]} respectively. Informally, the Arnold diffusion problem says that small perturbations can accumulate to large effects.

Recent results in the a priori unstable case include, ^{[8] [9] [10] [11] [12]} and in the a priori stable case. ^{[13] [14]}

In the context of the restricted three-body problem, Arnold diffusion can be interpreted in the sense that, for all sufficiently small, non-zero values of the eccentricity of the elliptic orbits of the massive bodies, there are solutions along which the energy of the negligible mass changes by a quantity that is independent of eccentricity. ^{[15] [16] [17]}

See also

• KAM theorem
• Nekhoroshev estimates

References

1. Arnold, Vladimir I. (1964). "Instability of dynamical systems with several degrees of freedom". Soviet Mathematics . 5: 581–585.
2. Florin Diacu; Philip Holmes (1996). Celestial Encounters: The Origins of Chaos and Stability. Princeton University Press. p. 193. ISBN   0-691-00545-1.
3. Pierre Lochak, (1999) Arnold diffusion; a compendium of remarks and questions In "Hamiltonian Systems with Three or More Degrees of Freedom" (S’Agar´o, 1995), C. Sim´o, ed, NATO ASI Series C: Math. Phys. Sci., Vol. 533, Kluwer Academic, Dordrecht (1999), 168–183.
4. Henk W. Broer, Mikhail B. Sevryuk (2007) KAM Theory: quasi-periodicity in dynamical systems In: H.W. Broer, B. Hasselblatt and F. Takens (eds.), Handbook of Dynamical Systems Vol. 3, North-Holland, 2010
5. Chierchia, Luigi; Gallavotti, Giovanni (1994). "Drift and diffusion in phase space". Annales de l'I.H.P.: Physique Théorique. 60: 1–144. MR   1259103. Zbl   1010.37039. (Erratum:  [Annales de l'I.H.P.: Physique Théorique.68: 135 (1998)]. If the erratum has been checked and does not affect the cited material, please replace {{ Erratum |...}} with {{ Erratum |...|checked=yes}}.)
6. Chen, Qinbo; de la Llave, Rafael (2022-03-09). "Analytic genericity of diffusing orbits in a priori unstable Hamiltonian systems". Nonlinearity. 35 (4). IOP Publishing: 1986–2019. arXiv: 2103.03847 . Bibcode:2022Nonli..35.1986C. doi: 10.1088/1361-6544/ac50bb . ISSN   0951-7715.
7. Mather, John N. (2012). "Arnold Diffusion by Variational Methods". Essays in Mathematics and its Applications. Berlin, Heidelberg: Springer Berlin Heidelberg. pp. 271–285. doi:10.1007/978-3-642-28821-0_11. ISBN   978-3-642-28820-3.
8. Bolotin, S; Treschev, D (1999-01-01). "Unbounded growth of energy in nonautonomous Hamiltonian systems". Nonlinearity. 12 (2). IOP Publishing: 365–388. Bibcode:1999Nonli..12..365B. doi:10.1088/0951-7715/12/2/013. ISSN   0951-7715. S2CID   250852828.
9. Cheng, Chong-Qing; Yan, Jun (2004-07-01). "Existence of Diffusion Orbits in a priori Unstable Hamiltonian Systems". Journal of Differential Geometry. 67 (3). International Press of Boston. doi: 10.4310/jdg/1102091356 . ISSN   0022-040X.
10. Delshams, Amadeu; de la Llave, Rafael; M-Seara, Tere (2006). "A geometric mechanism for diffusion in Hamiltonian systems overcoming in the large gap problem: Heuristics and rigorous verification on a model". Mem. Am. Math. Soc. 179 (844). doi:10.1090/memo/0844. hdl: 2117/872 .
11. Gelfreich, Vassili; Turaev, Dmitry (2017-04-24). "Arnold Diffusion in A Priori Chaotic Symplectic Maps". Communications in Mathematical Physics. 353 (2). Springer Science and Business Media LLC: 507–547. Bibcode:2017CMaPh.353..507G. doi:10.1007/s00220-017-2867-0. hdl: 10044/1/44044 . ISSN   0010-3616. S2CID   253744630.
12. Gidea, Marian; Llave, Rafael; M‐Seara, Tere (2019-07-24). "A General Mechanism of Diffusion in Hamiltonian Systems: Qualitative Results". Communications on Pure and Applied Mathematics. 73 (1). Wiley: 150–209. doi:10.1002/cpa.21856. hdl: 2117/188944 . ISSN   0010-3640. S2CID   119150120.
13. Cheng, Chong-Qing (2019). "The genericity of Arnold diffusion in nearly integrable Hamiltonian systems". Asian Journal of Mathematics. 23 (3). International Press of Boston: 401–438. arXiv: 1801.02921 . doi:10.4310/ajm.2019.v23.n3.a3. ISSN   1093-6106. S2CID   119677951.
14. Kaloshin, Vadim; Zhang, Ke (2020-11-12). Arnold Diffusion for Smooth Systems of Two and a Half Degrees of Freedom (PDF). Princeton University Press. doi:10.1515/9780691204932. ISBN   978-0-691-20493-2.
15. Xia, Zhihong (1993). "Arnold diffusion in the elliptic restricted three-body problem". Journal of Dynamics and Differential Equations. 5 (2). Springer Science and Business Media LLC: 219–240. Bibcode:1993JDDE....5..219X. doi:10.1007/bf01053161. ISSN   1040-7294. S2CID   121370238.
16. Delshams, Amadeu; Kaloshin, Vadim; de la Rosa, Abraham; Seara, Tere M. (2018-09-05). "Global Instability in the Restricted Planar Elliptic Three Body Problem". Communications in Mathematical Physics. 366 (3). Springer Science and Business Media LLC: 1173–1228. doi:10.1007/s00220-018-3248-z. hdl: 2117/123338 . ISSN   0010-3616. S2CID   253752812.
17. Capiński, Maciej; Gidea, Marian (2021). "A general mechanism of instability in Hamiltonian systems: skipping along a normally hyperbolic invariant manifold". Communications on Pure and Applied Mathematics. doi: 10.1002/cpa.22014 .