8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Quantized Vortex Stability and Dynamics
in Superfluidity and Superconductivity
Weizhu Bao
Department of Mathematics
& Center for Computational Science and Engineering
National University of Singapore
Email: [email protected]
URL: http://www.math.nus.edu.sg/~bao
Collaborators:
β Qiang Du: Penn State U.; Yanzhi Zhang: FSU
β Alexander Klein, Dieter Jaksch: Oxford
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Outline
MotivationMathematical models
Central vortex states andstabilityVortex interactionand reduced dynamic laws
Numerical methodsNumerical results for vortex interaction
Conclusions
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Motivation
β’ Quantized Vortex: Particle-like (topological) defect β Zero of the complex scalar field,
β localized phase singularities with integer topological charge:
β Key of superfluidity: ability to support dissipationless flow
02)(arg,)(,0)( 0 β ==== β« β« Ξ Ξ
nd d e x x i Ο Ο Ο Ο Ο Ο Ο
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Motivation
β’ Existing in β Superconductors:
β’ Ginzburg-Landau equations (GLE)
β Liquid helium:β’ Two-fluid model
β’ Gross-Pitaevskii equation (GPE)
β Bose-Einstein condensation (BEC):β’ Nonlinear Schroedinger equation (NLSE) or GPE
β Nonlinear optics & propagation of laser beams
β’ Nonlinear Schroedinger equation (NLSE)β’ Nonlinear wave equation (NLWE)
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Mathematical models
β’ Ginzburg-Landau equation (GLE):Superconductivity, nonlinear heat flow, etc.
β’ Gross-Pitaevskii equation (GPE): nonlinear optics, BEC, superfluidity
β’ Nonlinear wave equation (NLWE): wave motion
β Here
( )2 2
2
1( ) , , 0,t V x x R t Ο Ο Ο Ο
Ξ΅ = Ξ + β β >
: complex-valued wave function,
0: constant,( ) : real-valued external potentialV x
Ο
Ξ΅ >
( )2 2
21 ( ) , , 0,t i V x x R t Ο Ο Ο Ο Ξ΅ β = Ξ + β β >
( )2 2
2
1( ) , , 0,
tt V x x R t Ο Ο Ο Ο
Ξ΅ = Ξ + β β >
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Mathematical models
β’ `FreeEnergyβ or Lyapunov functional:
β’ Dispersive system(GPE): β Energy conservation:
β Density conservation:
β Admits particle like solutions: solitons, kinks & vortices
β’ Dissipative system(GLE):
β Energy diminishing, etc.
( )2
22 2
2
1( ) ( ) ,
2 E V x dxΟ Ο Ο
Ξ΅ β
β‘ β€= β + ββ’ β₯β£ β¦
β«
0),()( 0 β₯β‘ t E E Ο Ο
( ) 0,0|)(||),(|2
2
0
2 β₯β‘ββ« β
t xd xt x
Ο Ο
( )
*
E
i t
Ο Ξ΄ Ο
Ξ΄Ο
ββ = β
β
( )
*
E
t
Ο Ξ΄ Ο
Ξ΄Ο
β= β
β
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Two kinds of vortices
`Bright-tailβ vortex: GLE, GPE & NLWE (Μorder parameterβ)
β Time independent case (Neu, 90β):
β Vortex solutions:
β Asymptotic results
( ) 1, when , ( , ) 1, , ( . . ),imV x x x t x e g eΞΈ Ο Ο β β β β β β β β
1)(,1 β‘= xV
Ξ΅
ΞΈ Ο Ο in
nn er f x x )()()( ==
.1)(,0)0(
,0,0)())(1()()(1
)( 2
2
2
=β=
β<<=β+ββ²+β²β²
nn
nnnnn
f f
r r f r f r f
r
nr f
r
r f
β©β¨
β§
ββ+β
β+
β
+
.), / 1(2 / 1
,0),(
)( 422
2||||
r r Or n
r r Oar
r f
nn
n
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`Bright-tailβ vortex
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Two kinds of vortices
`Dark-tailβ vortex: BEC (wave function)
β Center vortex states:
β Asymptotic results
( , ) ( ) ( )n ni t i t in
n n x t e x e f r e
ΞΌ ΞΌ ΞΈ Ο Ο β β= =
2 23
2
2
0
( )( ) ( ) ( ), 0 ,
2
(0) 0, ( ) 0, 2 ( ) 1
nn n n n
n n n
d df r n r f r r f r f r r
dr dr r
f f f r r dr
ΞΌ Ξ²
Ο
β
β ββ β= β + + + < < ββ β β β
β β β β
= β = =β«
2
| | | | 2
| |
( ), 0,( )
, .
n n
n n r
a r O r r f r
b r e r
+
β
β§ + ββͺβ
β¨ β ββͺβ©
222 2 2| |
| | , , 0, | | 12
t
xi x R t dxΟ Ο Ο Ξ² Ο Ο Ο Ο = βΞ + + β > = =β«
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`Dark-tailβ vortex
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`Dark-tailβ vortex line in 3D
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Stability of vortices
β’ Data chosen
β’ Results (Bao,Du & Zhang, Eur. J. Appl. Math., 07β)
β For GLE or NLWE with initial data perturbed
β’ n=1: velocity density
β’ N=3: velocity density
β For NLSE with external potential perturbedβ’ n=1: velocity density
β’ N=3: velocity density
β’ Conclusion next
)noise()()()),,((1),(,1 0 +=+β‘= x xt xW t xV h
n
Ο Ο Ξ΅
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Conclusion of Stability
β’ For GLEor NLWE: β under perturbation either in initial data or in external potential
β’ |n|=1: dynamically stable,
β’ |n|>1: dynamically unstable. Splitting pattern depends on perturbation,when t >>1, it becomes n well-separated vortices with index 1 or β1.
β’ For NLSEor GPE:
β under perturbation in initial dataβ’ dynamically stable: Angular momentum expectation is conserved!!
β under perturbation in external potential
β’ |n|=1: dynamically stable, backβ’ |n|>1: dynamically unstable. Vortex centers can NOT move out of core size.
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Vortex interaction
β’ For Μ bright-tailβ vortex:
β’ For Μ dark-tailβ vortex
β Well-separate
β Overlapped
0 0 0
0
1 1
( ) ( ) ( , ) j j
N N
m j m j j
j j
x x x x x y yΟ Ο Ο = =
= β = β ββ β
0
1
( , ) ( , ) / || || j
N
n j j
j
x y x x y yΟ Ο =
= β β β’β
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Reduced dynamic laws
β’ For `bright-tailβ vortex β For GLE
β For GPE
β For NLWE
21,
0
( ) ( ) ( )( ) : 2 , 0
( ) ( )
(0) , 1 .
N j j l
j j l
l l j j l
j j
d x t x t x t v t m m t
dt x t x t
x x j N
ΞΊ ΞΊ = β
β= = β₯
β
= β€ β€
β
21,
0
( ) ( ( ) ( ))( ) : 2 0,
( ) ( )
0 1(0) 1 ;
1 0
N j j l
j l
l l j j l
j j
d x t J x t x t v t m t
dt x t x t
x x j N J
= β
β= = β₯
β
β β= β€ β€ = β β
ββ β
β
2
221,
0 ' 0
( ) ( ) ( )2 , 0
( ) ( )
(0) , (0) , 1 .
N j j l
j l
l l j j l
j j j j
d x t x t x t m m t
dt x t x t
x x x v j N
ΞΊ = β
β= β₯
β
= = β€ β€
β
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Existing mathematical results
β’ For GLE (or NLHE): β Pairs of vortices with like (opposite) index undergo a replusive (attractive)
interaction: Neu 90, Pismen & Rubinstein 91, W. E, 94, Bethual, etc.
β Energy concentrated at vortices in 2D & filaments in 3D: Lin 95--
β Vortices are attracted by impurities: Chapman & Richardson 97, Jian 01
β’ For NLSE: β Vortices behave like point vortices in ideal fluid: Neu 90
β Obeys classical Kirchhoff law for fluid point vortices: Lin & Xin 98
β Equations for vortex dynamics & radiation: Ovchinnikov& Sigal 98--; Jerrard,Bethual, etc.
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Conservation laws
β’ Mass center Lemma The mass center of the N vortices for GLE is conserved
Lemma The mass center of the N vortices for NLWE is conserved
if initial velocity is zero and it moves linearly if initial velocity isnonzero
1
1
( ) : ( )
N
j j x t x t N =
=
β
0
1 1 1
1 1 1( ) : ( ) (0) : (0)
N N N
j j j j j j
x t x t x x x N N N = = =
= β‘ = =
β β β
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Conservation laws
β’ Signed mass center
Lemma The signed mass center of the N vortices for NLSE is conserved
1
1( ) : ( )
N
j j
j
x t m x t N =
= β
0
1 1 1
1 1 1( ) : ( ) (0) : (0)
N N N
j j j j j j
j j j
x t m x t x m x m x N N N = = =
= β‘ = =β β β
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Analytical Solutions
β’ like vortices on acircle (Bao, Du & Zhang, SIAP, 07β)
β’ Analytical solutions for GLE figure
β’ Analytical solutions for NLSEfigure next
( 2) N β₯0
0
2 2cos , sin , 1, 1 j j
j j x a m m j N
N N
Ο Ο β ββ β β β= = = Β± β€ β€β β β ββ β
β β β β β β
2 2( 1) 2 2( ) cos , sin j
N j j x t a t
N N
Ο Ο
ΞΊ
β β ββ β β β= + β β β ββ β
β β β β β β
2 2
2 1 2 1( ) cos , sin j
j N j N x t a t t
N a N a
Ο Ο β β β ββ β β β= + +β β β ββ β
β β β β β β
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N=2 N=3
back
N=4
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N=2 N=3back
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Analytical Solutions
β’ like vortices on acircle and its center (Bao,Du&Zhang, SIAP, 07β)
β’ Analytical solutions for GLE figure
β’ Analytical solutions for NLSE figure next
( 3) N β₯
0 0 2 20; cos , sin , 1 1
1 1 N j
j j x x a j N
N N
Ο Ο β ββ β β β= = β€ β€ ββ β β ββ ββ ββ β β β β β
2 2
2 2 2 2( ) 0; ( ) cos , sin
1 1 N j
j N j N x t x t a t t
N a N a
Ο Ο β β β ββ β β β= = + +β β β ββ ββ ββ β β β
β β
2 2 2 2( ) 0; ( ) cos , sin , 1 1
1 1 N j
N j j x t x t a t j N
N N
Ο Ο
ΞΊ
β ββ β β β= = + β€ β€ ββ β β ββ ββ ββ β β β β β
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N=3 N=4back
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N=3 N=4back
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Analytical Solutions
β’ Twooppositevortices (Bao, Du & Zhang, SIAP, 07β)
β’ Analytical solutions for GLEfigure
β’ Analytical solutions for NLSE figure next
( ) ( )( )0 0
1 2 0 0 1 2cos , sin , 1 x x a m mΞΈ ΞΈ = β = = β =
( ) ( )( )2
1 2 0 0
2( ) ( ) cos , sin x t x t a t ΞΈ ΞΈ
ΞΊ = β = β
( ) ( )( )0
0 0( ) sin , cos , 1, 2 j j
t x t x j
aΞΈ ΞΈ = + β =
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Analytical Solutions
β’ opposite vortices on acircle and its center
β’ Analytical solutions for GLEfigure
β’ Analytical solutions for NLSE figure next
( 3) N β₯0 0 2 20 ( ); cos , sin ( ), 1 1
1 1 N j
j j x x a j N
N N
Ο Ο β ββ β β β= β = + β€ β€ ββ β β ββ ββ ββ β β β β β
2 2
2 4 2 4( ) 0; ( ) cos , sin
1 1 N j
j N j N x t x t a t t
N a N a
Ο Ο β β β ββ β β β= = + +β β β ββ ββ ββ β β β β β
2 2( 4) 2 2( ) 0; ( ) cos , sin , 1 1
1 1 N j
N j j x t x t a t j N
N N
Ο Ο
ΞΊ
β β ββ β β β= = + β€ β€ ββ β β ββ ββ ββ β β β β β
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N=3 N=4
back
N=5
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N=3 N=4
back
N=5
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Numerical difficulties
β’ Numerical difficulties: β Highly oscillatory nature in the transverse direction: resolution
β Quadratic decay rate in radial direction: large domain
β For NLSE, more difficulties:
β’ Time reversible
β’ Time transverse invariant
β’ Dispersive equation
β’ Keep conservation laws in discretized level
β’ Radiation
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Numerical methods
β’ For Μ bright-tailβ vortex(Bao,Du & Zhang, Eur. J. Appl. Math., 07β)
β Apply a time-splitting technique: decouple nonlinearity
β Adapt polar coordinate: resolve solution in transverse better
β Use Fourier pesudo-spectral discretization in transverse β Use 2nd or 4th order FEM or FDM in radial direction
For Μ dark-tailβ vortex (Bao & Zhang, M3AS, 05β)
β Apply a time-splitting technique: decouple nonlinearity
β Use Fourier pseudo-spectral discretization
β Use generalized Laguerre-Hermite pseudo-spectral method
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Vortex dynamics & interaction
β’ Data chosen (Bao, Du & Zhang, SIAM, J. Appl. Math., 07β)
β’ Two vortices with like winding numbers
β For GLE: velocity density
β For GPE: velocity density
β Trajectory
β’ Conclusion next
ββ==
=β=β‘= N
j
j
N
j
jn nm x x xt xV j
11
0 ,)()(,1),(,1
Ο Ο Ξ΅
)0,(),0,(,1,1,2 2121 a xa xnn N β=====
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GLE GPE NLWE
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Conclusion of interaction
β’ For GLE(Bao, Du & Zhang, SIAP, 07β)
β Undergo a repulsive interaction
β Core size of the two vortices will well separated
β Energy decreasing:
β’ For NLSE (Bao, Du & Zhang, SIAP, 07β)
β Behave like point vortices in ideal fluid
β The two vortex centers move almost along a circle
β Energy conservation & radiation back
β’ For NLWE (Bao & Zhang, 07β)
β Similar as GLE but with different speed
βββ t x E t x E )),((2)),(( 1
Ο Ο
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Vortex dynamics & interaction
β’ Two vortices with opposite winding numbers
β For GLE: velocity density β For NLSE:
β’ Case 1: velocity density
β’ Case 2: velocity density
β Trajectory
β’ Conclusion next
)0,(),0,(,1,1,2 2121 a xa xnn N β==β===
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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NLSEGLENLSE NLWE
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Conclusion of interaction
β’ For GLE(Bao, Du & Zhang, SIAP, 07β)
β Undergo an attractive interaction & merge at finite time
β Energy decreasing:
β’ For GPE (Bao, Du & Zhang, SIAP, 07β)
β depends on initial distance of the two centers
β’ Small: merge at finite time & generate shock wave
β’ Large: move almost paralleling & donβt merge, solitary wave β Energy conservation & radiation
β Sound wave generation back
For NLWE (Bao & Zhang, 07β)
β Undergo an attractive interaction & merge at finite time
βββ t t x E ,0)),((
Ο
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Reduced dynamic laws
For Μ dark-tailβ vortex in BEC(Klein, Jaksch, Zhang & Bao, PRA, 07β)
β For linear with harmonic potential
β’ N=1:
β’ Vortex pair:β’ Vortex dipole:
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Reduced dynamic laws
β For weak nonlinear case
β’ Vortex pair
β’ Vortex dipole
β’ Vortex tripole
β For strong interaction: ???
8/3/2019 Weizhu Bao- Quantized Vortex Stability and Dynamics in Superfluidity and Superconductivity
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Conclusions
β’ Analytical results for reduced dynamical laws β Mass center is conserved in GLE
β Signed mass center is conserved in GPE
β Solve analytically for a few types initial data
β’ Numerical results β Study numerically vortex dynamics in GLE, GPE, NLWE & NLSE
β’ Stability of a vortex with different winding number
β’ Interaction of vortex pair, vortex dipole, vortex tripole, β¦.