leonidrudenko - tum · 2009. 8. 21. · rudenko malfliet-tjonpotential †...
TRANSCRIPT
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Numerical solution of the three body scatteringproblem
Leonid Rudenko
Department of Computational Physics, St Petersburg State University
3 April, 2009
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Outline
• Introduction• The Three-body scattering problem
• Faddeev Equation• Solution expansion• Malfliet-Tjon potential
• Numerical calculations: eigenvalues, eigenfunctions,geometrical connections
• Conclusions
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Introduction
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Introduction
• Expanding of the tree body wave function• Basis of hyperspherical adiabatic harmonics• The standard projection procedure leads to effectiveequations for the expansion coefficients
• How can be solved?• Have to find out properties of the basis functions
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Introduction
• Geometrical connections Aij = 〈φi , ∂ρφj〉• Develop a formalism to study different models
- scattering of a particle off a two body bound state- scattering of a particle off a resonant state of a pair ofparticles
• Investigate eigenvalues λk , eigenfunctions φk , andgeometrical connections Aij of the operator
h(ρ) = −ρ−2∂θ + V (ρ cos θ).
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Faddeev Equation in {ρ, θ}Coordinates
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Faddeev equation in {ρ, θ}coordinates
The Faddeev s-wave equation in polar coordinates(−∂2
ρ −14ρ2
)U(ρ, θ) +
(− 1
ρ2∂2
θ + V (ρ cos θ)
)U(ρ, θ)−
−EU(ρ, θ) = −V (ρ cos θ)
√34
∫ θ+(θ)
θ−(θ)dθ′ U(ρ, θ′)
where θ+(θ) = π/2− |π/6− θ| and θ−(θ) = |π/3− θ|
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Faddeev equation in {ρ, θ}coordinates
The boundary conditions should be imposed for the scatteringsolution:• Regularity of the solution
U(0, θ) = U(ρ, 0) = U(ρ, π/2) = 0
• Asymptotics as ρ →∞
U(ρ, θ) ∼ ϕ(x)ρ1/2 sin(qy)/q +
+a(q)ϕ(x)ρ1/2 exp(iqy) + A(θ,E ) exp(i√Eρ),
where x = ρ cos θ.
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Faddeev equation in {ρ, θ}coordinates
• The bound-state wave function of the two body targetsystem ϕ(x) obeys the equation
{−∂2x + V (x)}ϕ(x) = εϕ(x)
• It is assumed that the discrete spectrum of the Hamiltonian−∂2
x + V (x) consists of one negative eigenvalue ε at most
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Basis functions
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Expansion basis
• As basis we choose the eigenfunctions set of the operatorh(ρ)
(−ρ−2∂2θ + V (ρ cos θ)
)φk(θ|ρ) = λk(ρ)φk(θ|ρ)
• ρ is an external parameter for h(ρ)
• EV and EF of h(ρ) inherit parametrical dependence on ρ
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Spectral properties
• The main spectral properties of the operator h(ρ) asρ →∞ and of the two body Hamiltonian −∂ 2
x + V (x)
λ = limρ→∞λ0(ρ) = ε,
φ0(θ|ρ) =√
ρϕ(ρ cos θ)(1 + O(ρ−µ))
• Excited states φk(θ|ρ), k ≥ 1, when ρ →∞ theasymptotic behavior is given by the formulas
λk(ρ) ∼(2kρ
)2
,
φk(θ|ρ) ∼ 2√πsin(2kθ)
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Perturbation Theory
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Perturbation theory - introduction
• If the parameter ρ is large the support of the potentialV (ρ cos θ) is small on the interval [0, π/2]
• The estimates for EV and EF of the operator h(ρ) can beobtained by the perturbation theory considering thepotential V (ρ cos θ) as a small perturbation
λk ∼ λ0k + λ1
k ,
φk(θ|ρ) ∼ φ0k(θ|ρ) + φ1
k(θ|ρ)
• The leading terms λ0k and φ0
k for k ≥ 1 are given by
λ0k = (2k)2/ρ2,
φ0k(θ|ρ) =
2√πsin(2kθ)
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Correction terms
• The first order correction terms λ1k and φ1
k are defined interms of the matrix elements of the potential V (ρ cos θ)
Vnk(ρ) = 〈φ0n|V |φ0
k〉 =
∫ π/2
0dθ φ0
n(θ|ρ)V (ρ cos θ)φ0k(θ|ρ)
• As the model situation, the function V (x) is taken in theform of Yukawa potential
V (x) = Cexp(−µx)
x
where C and µ are some parameters.
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Calculation of corrections
• As we set ρ →∞, we can approximately calculate integral
Vnk(ρ) ∼ (−1)n+k 16nkCπ
[1− exp(−µR)(1 + µR)]
µ21ρ3
.
• The first order correction term λ1k is
λ1k = Vkk ∼ ρ−3
• The second order correction term λ2k is
λ2k =
∑
n 6=k
|Vnk |2λ
(0)k − λ
(0)n
,
λ2k ∼ ρ−4
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Calculation of corrections
• For eigenfunctions the first correction term is given by
φ1k =
∑
n 6=k
Vnk
λ(0)k − λ
(0)n
φ0n ∼ ρ−1
• From equation(− 1
ρ2∂2
θ + V (ρ cos θ)
)φk(θ|ρ) = λk(ρ)φk(θ|ρ)
one can obtain formula for Aij
Aij =〈φi | ∂V
∂ρ |φj〉λi − λj
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Aij
• Rough calculation of Aij leads to dependence
Aij ∼ ρ−2, i , j 6= 0
Aij ∼ ρ−5/2, i = 0 or j = 0
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Solution Expansion
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Solution expansion
• The operator h(ρ) is Hermitian on [0, π/2] interval and itseigenfunction set {φk(θ|ρ)}∞0 is complete.
U(ρ, θ) = φ0(θ|ρ)F0(ρ) +∑
k≥1φk(θ|ρ)Fk(ρ)
• Substituting this expansion in Faddev equation andprojecting on basis functions lead to the following systemof equations for Fk(ρ), k = 0, 1, ...
(−∂2
ρ −14ρ2
+ λk(ρ)− E)Fk(ρ) =
∞∑
i=0
(2Aki
∂Fi (ρ)
∂ρ+ Bki (ρ)Fi (ρ)−Wki (ρ)Fi (ρ)
)
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Solution expansion
• The nonadiabatical matrix elements Aki (ρ),Bki (ρ) andpotential coupling matrix Wki (ρ) are given by integrals
Aki (ρ) = 〈φk | ∂ρφi 〉 =
∫ π/2
0dθφ∗k(θ|ρ)
∂φi (θ|ρ)
∂ρ,
Bki (ρ) = 〈φk | ∂ 2ρ φi 〉 =
∫ π/2
0dθφ∗k(θ|ρ)
∂ 2φi (θ|ρ)
∂ρ 2 ,
Wki (ρ) =
√34
∫ π/2
0dθφ∗k(θ|ρ)V (ρ cos θ)
∫ θ+(θ)
θ−(θ)dθ′φi (θ
′|ρ)
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Solution expansion
• Presence of first derivative F ′i (ρ) in the right part of theexpression
• Matrix form of equation(−∂2
ρ −14ρ2
+ Λ(ρ)− E)F (ρ) = 2AF ′(ρ)+(B−W )F (ρ)
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Solution expansion
• Transform equation in form
F ′′(ρ) + PF ′(ρ) + QF (ρ) = 0
where P = 2A and Q =(
14ρ2 − Λ(ρ) + E + B −W
)are
two-dimensional infinite matrices• Introduce
F = UG
and elements of G are new unknown quantities
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Solution expansion
UG ′′ +(2U ′ + PU
)G ′ +
(U ′′ + PU ′ + QU
)G = 0
• Equation for matrix U
U ′ = −12PU = −AU
• As ρ →∞U(ρ) = I +
∫ ∞
ρAUdρ
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Solution expansion
• Form without first derivative
UG ′′ +(−12P ′ − 1
4P2 + Q
)UG = 0
• Substitute expressions for P and Q
G ′′ + U−1(−A′(ρ)− A2(ρ) +14ρ2
−−Λ(ρ) + E + B −W )UG = 0
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Solution expansion
• As ρ →∞ asymptotic behavior U(ρ) ∼ I(−∂2
ρ −14ρ2
I + Λ(ρ)− E)G =
=(−A′(ρ)− A2(ρ) + B(ρ)−W (ρ)
)G
• The right hand side terms vanish for large ρ faster thanρ−2. Hence this terms can be neglected.
(−∂2
ρ −14ρ2
+ λask (ρ)− E
)Gk(ρ) = 0
here λas0 (ρ) = ε and λas
k (ρ) = (2k)2/ρ 2, k ≥ 1
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Solution expansion
• Solutions to these equations with appropriate asymptoticscan be expressed in terms of the Bessel (Y , J) functionsand the Hankel (H(1)) functions of the first kind asfollowing
G0(ρ) ∼√
πqρ
2Y0(qρ)− J0(qρ)√
2q+
a0(q)
√πqρ
2H(1)0 (qρ)e iπ/4
Gk(ρ) ∼ ak(E )
√π√Eρ
2H(1)2k (
√Eρ)e i(π/4+kπ)
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Malfliet-Tjon Potential
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Malfliet-Tjon potential
• A potential, which describes the modeling nucleon-nucleoninteraction acting in the triplet state with the spin 3/2
• Form of the Yukawa terms superposition
V (x) = V1exp(−µ1x)
x+ V2
exp(−µ2x)
x
with parameters listed in the table
Coefficient ValueV1 −626, 885MeVV2 1438, 72MeVµ1 1, 55 Fm−1
µ2 3, 11 Fm−1
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Malfliet-Tjon potential
0 1 2 3
-2
-1
0
1
2
3
V(x
), Fm
^(-2
)
x, Fm
V(x)
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Unit system
• Proton-neutron interaction(− ~
2
2µ∂2x + V (x)
)ψ(x) = Eψ(x),
• Reduced mass
µ =mpmn
mp + mn' m2
2m=
m2
, mp ' mn = m
(−∂2
x +m~2
V (x)− m~2
E)
ψ(x) = 0
• [V ] = [E ] = MeV
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Unit system
•~2
m' 41, 47 Fm2 ∗MeV
• Obtain equation(−∂2
x + V (x)− E)
ψ(x) = 0
where [V ] = [E ] = Fm−2
• Set x = ρ cos θ in polar coordinates and ρ is parameter
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
ρ = 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6-5
0
5
10
15
20
25
30
V(rho
*cos
(The
ta))
Theta
V(rho*cos(Theta)), rho=1
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
ρ = 10
1,2 1,4 1,6-2
-1
0
1
2
3
V(rho
*cos
(The
ta))
Theta
V(rho*cos(Theta)), rho=10
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
ρ = 100
1,52 1,53 1,54 1,55 1,56 1,57 1,58-2
-1
0
1
2
3
4
V(rho
*cos
(The
ta))
Theta
V(rho*cos(Theta)), rho=100
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Numerical Calculations
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Numerical calculations
• Finite-difference approach
−φk(θ − h) + 2φk(θ)− φk(θ + h)ρ 2h 2 +
+V (ρ cos θ)φk(θ) = λkφk(θ)
where h = θi+1 − θi , i = 1, ...,N and N ∼ 100000• Boundary conditions
φk(0) = φk(π/2) = 0
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Software
• CLAPACK• Intel Math Kernel Library 10.0.1 for Unix• ’DSTEVX’: computes selected eigenvalues and, optionally,eigenvectors of a real symmetric tridiagonal matrix.Eigenvalues and eigenvectors can be selected by specifyingeither a range of values or a range of indices.
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Eigenvalues
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Asymptotics
• k = 0lim
ρ→∞λ0(ρ) = ε
• k ≥ 1
λk(ρ) ∼(2kρ
)2
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
λ0(ρ)
0 10 20 30 40-0,08
-0,06
-0,04
-0,02
0,00
0,02
0,04
rho
lambda0
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
λ10(ρ)
0 2 4 6 8 10 12 14 16 18 20
0
20
40
60
80
100
rho
lambda10 asymptotic
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Eigenvalues
0 5 10 15 20 25 30 35 40-0,10
-0,05
0,00
0,05
0,10
0,15
0,20
0,25
0,30
Eigen
values
rho
lambda0 lambda1 lambda2 lambda3 lambda4 lambda5
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Deviation from asymptotics
• ρ ∼ 10 – deviation is big and varies from 10% up to 90%.For small k the absolute deviation is bigger than for big k .
• ρ ∼ 100 – deviation is about 5− 7%• ρ = 700 – deviation is less than 1%• ρ ∼ 1000 – deviation is about 0, 7%
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Eigenfunctions
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60,0
0,2
0,4
0,6
0,8
1,0
1,2
1,4
Theta
phi0(Theta), rho=1
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 3
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60,0
0,2
0,4
0,6
0,8
1,0
1,2
1,4
Theta
phi0(Theta), rho=3
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 5
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60,0
0,2
0,4
0,6
0,8
1,0
1,2
1,4
Theta
phi0(Theta), rho=5
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 10
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60,0
0,2
0,4
0,6
0,8
1,0
1,2
1,4
1,6
1,8
Theta
phi0(Theta), rho=10
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 30
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60,0
0,5
1,0
1,5
2,0
2,5
3,0
Theta
phi0(Theta), rho=30
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60
2
4
6
8
10
12
14
16
18
Theta
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 3
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60
2
4
6
8
10
12
14
16
18
Theta
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 5
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60
2
4
6
8
10
12
14
16
18
Theta
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 10
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60
2
4
6
8
10
12
14
16
18
Theta
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 30
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60
2
4
6
8
10
12
14
16
18
Theta
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 100
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60
2
4
6
8
10
12
14
16
18
Theta
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 300
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60
2
4
6
8
10
12
14
16
18
Theta
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 500
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60
2
4
6
8
10
12
14
16
18
Theta
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ), ρ = 1000
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60
2
4
6
8
10
12
14
16
18
Theta
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Step-by-step
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60123456789
101112131415161718
Theta
rho=1 rho=3 rho=5 rho=10 rho=30 rho=100 rho=300 rho=500 rho=1000
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Step-by-step
1,48 1,50 1,52 1,54 1,56 1,580123456789
101112131415161718
Theta
rho=1 rho=3 rho=5 rho=10 rho=30 rho=100 rho=300 rho=500 rho=1000
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φ0(θ): conclusions
• As ρ →∞ eigenfunction φ0 transforms into δ-function• Computational problems: decreasing of spacing, time ofcomputation, size of data, useless zero-area
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φk(θ), k ≥ 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6
-1,0
-0,5
0,0
0,5
1,0
Theta
k=1 k=2 k=3 k=4 k=5
phi_k(Theta), rho=1
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φk(θ), k ≥ 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6
-1,0
-0,5
0,0
0,5
1,0
Theta
k=1 k=2 k=3 k=4 k=5
phi_k(Theta), rho=3
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φk(θ), k ≥ 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6
-1,0
-0,5
0,0
0,5
1,0
Theta
k=1 k=2 k=3 k=4 k=5
phi_k(Theta), rho=5
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φk(θ), k ≥ 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6
-1,0
-0,5
0,0
0,5
1,0
Theta
k=1 k=2 k=3 k=4 k=5
phi_k(Theta), rho=10
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φk(θ), k ≥ 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6
-1,2
-1,0
-0,8
-0,6
-0,4
-0,2
0,0
0,2
0,4
0,6
0,8
1,0
1,2
Theta
k=1 k=2 k=3 k=4 k=5
phi_k(Theta), rho=30
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φk(θ), k ≥ 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6
-1,2
-1,0
-0,8
-0,6
-0,4
-0,2
0,0
0,2
0,4
0,6
0,8
1,0
1,2
Theta
k=1 k=2 k=3 k=4 k=5
phi_k(Theta), rho=100
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φk(θ), k ≥ 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6
-1,2
-1,0
-0,8
-0,6
-0,4
-0,2
0,0
0,2
0,4
0,6
0,8
1,0
1,2
Theta
k=1 k=2 k=3 k=4 k=5
phi_k(Theta), rho=300
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φk(θ), k ≥ 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6
-1,2
-1,0
-0,8
-0,6
-0,4
-0,2
0,0
0,2
0,4
0,6
0,8
1,0
1,2
Theta
k=1 k=2 k=3 k=4 k=5
phi_k(Theta), rho=500
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
φk(θ), k ≥ 1
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6
-1,2
-1,0
-0,8
-0,6
-0,4
-0,2
0,0
0,2
0,4
0,6
0,8
1,0
1,2
Theta
k=1 k=2 k=3 k=4 k=5
phi_k(Theta), rho=1000
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Step-by-step φ1(θ)
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6
-1,0
-0,5
0,0
0,5
1,0
Theta
rho=1 rho=3 rho=5 rho=10 rho=30 rho=100 rho=300 rho=500 rho=1000
phi1(Theta)
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Orthogonality and deviations
• Check orthogonality on each step• When does eigenfunction reach its asymptotic behavior?
maxθ|φk,ρ(θ)− sin(2kθ)|
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
ρ = 500k max deviation1 0, 0250559876972 0, 0500959372663 0, 0751038619274 0, 1000641228465 0, 1249612277836 0, 1497801114307 0, 174506106355... ...14 0, 34385374894015 0, 36736662188116 0, 39067726760717 0, 41377642115718 0, 43665543471219 0, 45930633612320 0, 481722165969
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Deviation in case k = 20, ρ = 500
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60,0
0,1
0,2
0,3
0,4
0,5
Theta
| phi_20 - sin(2k*Theta) |, k=20
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
ρ = 1000k max deviation1 0, 0125481819912 0, 0250943003823 0, 0376362974544 0, 0501721150345 0, 0626997003586 0, 0752170845527 0, 087722341482... ...14 0, 17475841034215 0, 18709854139916 0, 19941053702017 0, 21169197253418 0, 22394158383119 0, 23615787682420 0, 248338419864
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Deviation in case k = 20, ρ = 1000
0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60,00
0,05
0,10
0,15
0,20
0,25
Theta
| phi_k - sin(2k*Theta) |, k=20
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Geometrical connections
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Geometrical connections
• Off-diagonal matrix of geometrical connections A withelements
Aki (ρ) = 〈φk |φ′i 〉 =
∫ π/2
0dθ φ∗k(θ|ρ)
∂φi (θ|ρ)
∂ρ
• Determines behavior of right part of equation(−∂2
ρ −14ρ2
I + Λ(ρ)− E)G =
=(−A′(ρ)− A2(ρ) + B(ρ)−W (ρ)
)G
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Geometrical connections
•Aki =
〈φk | ∂V∂ρ |φi 〉
λk − λi
• Aki = −Aik and Akk = 0
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Aki , k = 0 or i = 0
500 1000 1500 20000,0
0,2
0,4
0,6
0,8
1,0
A01
rho
num. calc. O(rho^(-2,5)) O(rho^(-2))
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Aki , k 6= 0 and i 6= 0
500 1000 1500 20000
1
2
3
A12
rho
num. calc. O(rho^(-2)) O(rho^(-1,5))
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Aki , k 6= 0 and i 6= 0
500 1000 1500 2000-2,0
-1,8
-1,6
-1,4
-1,2
-1,0
-0,8
-0,6
-0,4
-0,2
0,0
A13
rho
num. calc. O(rho^(-2)) O(rho^(-1,5))
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
The last note about Aki
• The behavior of geometrical connections Aki is regular (nosingularity or special points) in case of Malfliet-Tjonpotential.
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Numericalsolution ofthe threebody
scatteringproblem
LeonidRudenko
Thank you!