Modeling of fractional dynamics using L´ evy walks - recent advances Marcin Magdziarz Hugo Steinhaus Center Faculty of Pure and Applied Mathematics Wroclaw University of Science and Technology, Poland Fractional PDEs: Theory, Algorithms and Applications ICERM, Brown University, June 2018 Marcin Magdziarz (Wroclaw) Modelling of fract. dynamics - L´ evy walks ICERM 2018 1 / 45
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Modeling of fractional dynamics using L vy walks - recent ......WF(t) = XN t i=1 J i Note that |R WF(t)| ≤ t. 0 0 t R WF (t) J 3 J 4 J 1 T 2 J 2 T 3 T 4 T 5 J 5 T 6 T 6 Marcin Magdziarz
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Modeling of fractional dynamics using Levy walks -
recent advances
Marcin Magdziarz
Hugo Steinhaus Center
Faculty of Pure and Applied Mathematics
Wrocław University of Science and Technology, Poland
Fractional PDEs: Theory, Algorithms and ApplicationsICERM, Brown University, June 2018
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 1 / 45
Outline
Examples of applications of Levy walks
Basic definitions of Levy walks
Asymptotic (diffusion) limits of multidimensional Levy walks
Corresponding fractional diffusion equations
Explicit densities in multidimensional case
Other results
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 2 / 45
Examples of applications of Levy walks
Light transport in optical materialsP. Barthelemy, P.J. Bertolotti, D.S. Wiersma, Nature 453, 495 (2008).
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 3 / 45
Examples of applications of Levy walks
Foraging patterns of animalsM. Buchanan, Nature 453, 714 (2008).
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 4 / 45
Examples of applications of Levy walks
Migration of swarming bacteriaG. Ariel et al., Nature Communications (2015).
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 5 / 45
Examples of applications of Levy walks
Blinking nanocrystalsG. Margolin, E. Barkai, Phys. Rev. Lett. 94, 080601 (2005)F.D. Stefani, J.P. Hoogenboom, E. Barkai, Physics Today, 62 (2009)Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 6 / 45
Examples of applications of Levy walks
Human travelD. Brockmann, L. Hufnagel, and T. Geisel, Nature 439, 462 (2006).
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 7 / 45
Basic definitions – 1D case
Waiting times: Ti , i = 1, 2, ... – sequence of iid positive randomvariables with power-law distribution P(Ti > t) ∝ 1
tα, α ∈ (0, 1).
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 8 / 45
Basic definitions – 1D case
Waiting times: Ti , i = 1, 2, ... – sequence of iid positive randomvariables with power-law distribution P(Ti > t) ∝ 1
tα, α ∈ (0, 1).
Jumps:Ji = ΛiTi
where Λi are iid random variables with
P(Λi = 1) = p, P(Λi = −1) = 1− p.
They govern the direction of the jumps (velocity v = 1). |Ti | = |Ji |.
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 8 / 45
Basic definitions – 1D case
Waiting times: Ti , i = 1, 2, ... – sequence of iid positive randomvariables with power-law distribution P(Ti > t) ∝ 1
tα, α ∈ (0, 1).
Jumps:Ji = ΛiTi
where Λi are iid random variables with
P(Λi = 1) = p, P(Λi = −1) = 1− p.
They govern the direction of the jumps (velocity v = 1). |Ti | = |Ji |.Number of jumps up to time t:
Nt = max{n ≥ 0 : T1 + ...+ Tn ≤ t}.
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 8 / 45
Definition: Wait-First Levy Walk – 1D case
RWF (t) =
Nt∑
i=1
Ji
Note that |RWF (t)| ≤ t.
0
0
t
RW
F(t)
J3
J4
J1
T2
J2
T3
T4
T5
J5
T6
J6T
1
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 9 / 45
Definition: Jump-First Levy Walk – 1D case
RJF (t) =
Nt+1∑
i=1
Ji
0
0
t
RJF
(t)
T1
T2
J2
T3
J3
T4
J4
T5
J5
T6
J6J
1
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 10 / 45
Definition: Standard Levy Walk – 1D case
R(t) =
Nt∑
i=1
Ji + (t − T (Nt))ΛNt+1,
where T (n) =∑
n
i=1 Ti . Note that |R(t)| ≤ t.
0
0
t
R(t)
J5
J1
T1
J2
T2
J3
T3
J4
T4
T5
J6
T6
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 11 / 45
Basic definitions – d -dimensional case
Waiting times: Ti , i = 1, 2, ... – sequence of iid positive randomvariables with power-law distribution P(Ti > t) ∝ 1
tα, α ∈ (0, 1).
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 12 / 45
Basic definitions – d -dimensional case
Waiting times: Ti , i = 1, 2, ... – sequence of iid positive randomvariables with power-law distribution P(Ti > t) ∝ 1
tα, α ∈ (0, 1).
Jumps in Rd :
Ji = ΛiTi
where Λi are iid unit random vectors in Rd with the distribution
Λ(dx) on d−dimensional sphere Sd . They govern the direction ofthe jumps in Rd (velocity v = 1). We have |Ti | = ‖Ji‖.
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 12 / 45
Basic definitions – d -dimensional case
Trajectory Distribution Λ on S2
−4 −2 0
x 105
−4
−2
0
2x 10
5
292.5o315o
337.5o
0o
22.5o
45o67.5o112.5o
135o
157.5o
180o
202.5o
225o
247.5o
90o
270o
0 2 4 6
x 105
0
2
4
6
x 105
292.5o315o
337.5o
0o
22.5o
45o67.5o112.5o
135o
157.5o
180o
202.5o
225o
247.5o
90o
270o
−2 0 2
x 105
−4
−2
0
2x 10
5
292.5o315o
337.5o
0o
22.5o
45o67.5o112.5o
135o
157.5o
180o
202.5o
225o
247.5o
90o
270o
a)
b)
c)
d)
e)
f)
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 13 / 45
Basic definitions – d -dimensional case
Wait-First Levy Walk in Rd
RWF (t) =
Nt∑
i=1
Ji
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 14 / 45
Basic definitions – d -dimensional case
Wait-First Levy Walk in Rd
RWF (t) =
Nt∑
i=1
Ji
Jump-First Levy Walk in Rd
RJF (t) =
Nt+1∑
i=1
Ji
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 14 / 45
Basic definitions – d -dimensional case
Wait-First Levy Walk in Rd
RWF (t) =
Nt∑
i=1
Ji
Jump-First Levy Walk in Rd
RJF (t) =
Nt+1∑
i=1
Ji
Standard Levy Walk in Rd
R(t) =
Nt∑
i=1
Ji + (t − T (Nt))ΛNt+1,
where T (n) =∑
n
i=1 Ti .
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 14 / 45
Diffusion limits of Levy walks – d -dimensional case
Theorem (Diffusion limit of Wait-First Levy walk)
The following convergence in distribution holds as n → ∞
RWF (nt)
n
d−→ L−α (S−1α (t)).
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 15 / 45
Diffusion limits of Levy walks – d -dimensional case
Theorem (Diffusion limit of Wait-First Levy walk)
The following convergence in distribution holds as n → ∞
RWF (nt)
n
d−→ L−α (S−1α (t)).
Here:
Lα(t) – d -dimensional α-stable Levy motion (limit of jumps) withFourier transform
ΦLα(t)(k) = exp
(
t
∫
Sd
|〈k , s〉|α(isgn(〈k , s〉) tan(πα/2) − 1)Λ(ds))
Λ(ds) - distribution of jump direction
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 15 / 45
Diffusion limits of Levy walks – d -dimensional case
Theorem (Diffusion limit of Wait-First Levy walk)
The following convergence in distribution holds as n → ∞
RWF (nt)
n
d−→ L−α (S−1α (t)).
Here:
Lα(t) – d -dimensional α-stable Levy motion (limit of jumps) withFourier transform
ΦLα(t)(k) = exp
(
t
∫
Sd
|〈k , s〉|α(isgn(〈k , s〉) tan(πα/2) − 1)Λ(ds))
Λ(ds) - distribution of jump direction
Sα(t) – α-stable subordinator (limit of waiting times)
S−1α (t) = inf{τ ≥ 0 : Sα(τ) > t}
Marcin Magdziarz (Wrocław) Modelling of fract. dynamics - Levy walks ICERM 2018 15 / 45
Diffusion limits of Levy walks – d -dimensional case
Theorem (Diffusion limit of Wait-First Levy walk)
The following convergence in distribution holds as n → ∞
RWF (nt)
n
d−→ L−α (S−1α (t)).
Here:
Lα(t) – d -dimensional α-stable Levy motion (limit of jumps) withFourier transform
ΦLα(t)(k) = exp
(
t
∫
Sd
|〈k , s〉|α(isgn(〈k , s〉) tan(πα/2) − 1)Λ(ds))
Λ(ds) - distribution of jump direction
Sα(t) – α-stable subordinator (limit of waiting times)