Pavel Str ánský ECT* Seminar* 13 January 2012 Institute of Particle and Nuclear Phycics, Faculty of Mathematics and Physics, Charles University in Prague, Czech Republic CHAOTIC DYNAMICS AND QUANTUM STATE PATTERNS IN COLLECTIVE MODELS OF NUCLEI Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México Collaborato rs: Michal Macek, Pavel Cejnar Alejandro Frank, Emmanuel Landa, Irving Morales Jan Dobeš Nuclear Research Institute, Řež, Czech Republic 1 / 674
47
Embed
Pavel Stránský ECT* Seminar* 13 January 2012 Institute of Particle and Nuclear Phycics, Faculty of Mathematics and Physics, Charles University in Prague,
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Pavel Stránský
ECT* Seminar*
13 January 2012
Institute of Particle and Nuclear Phycics, Faculty of Mathematics and Physics,Charles University in Prague, Czech Republic
CHAOTIC DYNAMICS AND QUANTUM STATE PATTERNS IN COLLECTIVE
MODELS OF NUCLEI
Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México
Collaborators:
Michal Macek, Pavel Cejnar
Alejandro Frank, Emmanuel Landa, Irving Morales
Jan DobešNuclear Research Institute, Řež, Czech Republic
1 / 674
1. Classical chaos- Stable x unstable trajectories- Poincaré sections: a manner of visualization- Fraction of regularity: a measure of chaos
2. Quantum chaos- Statistics of the quantum spectra, spectral correlations- 1/f noise: long-range correlations- Peres lattices: ordering of quantum states
3. Applications in the nuclear physics- Geometric collective model and Interacting boson model- Quantum – classical correspondence- Adiabatic separation of the collective and intrinsic motion
CHAOTIC DYNAMICS AND QUANTUM STATE PATTERNS IN COLLECTIVE
MODELS OF NUCLEI
2 / 674
1. Classical Chaos(analysis of trajectories)
3 / 674
Hamiltonian systemsState of a system: a point in the 4D phase space
Conservative system:
Trajectory restricted to 3D hypersurface
Connected with additional symetries
Integrals of motion:
Integrable system: Number of independent
integrals of motion
number of degrees of freedom
=Canonical transformation to action-angle variables
Quasiperiodic motion on a toroid
J1
J2
1. Classical chaos
Hamiltonian systemsState of a system: a point in the 4D phase space
Conservative system:
Trajectory restricted to 3D hypersurface
Connected with additional symetries
Integrals of motion:
Integrable system: Number of independent
integrals of motion
number of degrees of freedom
=Canonical transformation to action-angle variables
Quasiperiodic motion on a toroid
J1
J2
Chaotic behaviour: property of nonintegrable
systems
1. Classical chaos
y
x
px
px
Section at
y = 0
x
ordered case – “circles”
chaotic case – “fog”
We plot a point every time when the trajectory crosses the plane y = 0
Poincaré sections
1. Classical chaos
Generic conservative system of 2 degrees of freedom
Different initial conditions at the same energy
REGULAR area
CHAOTIC area
freg=0.611 x
px
Fraction of regularity
Measure of classical chaos
Surface of the section covered with regular trajectories
Total kinematically accessible surface of the section
1. Classical chaos
1. Lyapunov exponent
Divergence of two neighboring trajectories
2. SALI (Smaller Alignment Index)
• fast convergence towards zero for chaotic trajectories
• two divergencies
Quasiperiodic X unstable trajectories
Regular: at most polynomial divergence
Chaotic: exponential divergence
Classical chaos –Hypersensitivity to
the initial conditions
Ch. Skokos, J. Phys. A: Math. Gen 34, 10029 (2001); 37 (2004), 6269
1. Classical chaos
2. Quantum Chaos(analysis of energy spectra)
Semiclassical theory of chaos
2. Quantum chaos
Spectral density:
smooth part
given by the volume of the classical phase space
oscillating part
Gutzwiller formula(given by the sum of all classical periodic orbits and their repetitions)
The oscillating part of the spectral density can give relevant information about quantum chaos (related to the classical trajectories)
Unfolding:
A transformation of the spectrum that removes the smooth part of the level density
Note: Improved unfolding procedure using the Empirical Mode Decomposition method in: I. Morales et al., Phys. Rev. E 84, 016203 (2011)
E
Quantum chaos: Spectral statistics
P(s)
Gaussian Orthogona
lEnsemble
CHAOTIC systems
REGULAR system
Transformation
H T invariance
Angular momentum
R invariance
GOE Orthogonal SymmetricYESYES
nn/2 YES
GUE Unitary Hermitian NO
GSE Symplectic YES n/2 NO
Nearest-neighbor spacing distribution
level repulsion
no level interaction
Gaussian Unitary
Ensemble
Gaussian Symplectic
Ensemble
Ensembles of random matrices
O. Bohigas, M. J. Giannoni, C. Schmit, Phys. Rev. Lett. 52 (1984), 1M.V. Berry, M.Tabor, Proc. Roy. Soc. A 356, 375 (1977)
2. Quantum chaos
Wigner
P(s)
s
Poisson
CHAOTIC systemREGULAR system
Brodydistributionparameter
- Tool to test classical-quantum correspondence
- Measure of chaoticity of quantum systems- Artificial interpolation between Poisson and GOE distribution
Spectral statistics
Nearest-neighbor spacing distribution
2. Quantum chaos
Schrödinger equation:(for wave function)
Helmholtz equation:(for intensity of el. field)
Quantum chaos - examples
2. Quantum chaos
They are also extensively studied
experimentally
Billiards
Riemann function:
Prime numbers
Riemann hypothesis:All points z(s)=0 in the complex plane lie on the line s=½+iy (except trivial zeros on the real exis s=–2,–4,–6,…)
GUE
Zeros of function
Quantum chaos - applications
2. Quantum chaos
GOE
Correlation matrix of the human EEG signal
P. Šeba, Phys. Rev. Lett. 91 (2003), 198104
Quantum chaos - applications
2. Quantum chaos
1/f noise
Power spectrum
A. Relaño et al., Phys. Rev. Lett. 89, 244102 (2002)E. Faleiro et al., Phys. Rev. Lett. 93, 244101 (2004)
CHAOTIC system = 1 = 2
Direct comparison of 3 measures of chaos
REGULAR system
= 2
= 1
1 = 0
2
3
4
n = 0k
k
- Fourier transformation of the time series constructed from energy levels fluctuations
J. M. G. Gómez et al., Phys. Rev. Lett. 94, 084101 (2005)
Ubiquitous in the nature (many time signals or space characteristics of complex systems have 1/f power spectrum)
2. Quantum chaos
Peres lattices Quantum system:
A. Peres, Phys. Rev. Lett. 53, 1711 (1984)
Infinite number of of integrals of motion can be constructed (time-averaged operators P):
nonintegrable
E
<P>
regular
E
Integrable
<P>
chaoticregular
B = 0 B = 0.445
Lattice: energy Ei versus value of
lattice always ordered for any operator P
partly ordered, partly disordered
2. Quantum chaos
3. Application to the collective models of nuclei
Surface of homogeneous nuclear matter:
Monopole deformations = 0
Geometric collective model
(even-even nuclei – collective character of the lowest excitations)
- Does not contribute due to the incompressibility of the nuclear matter
Dipole deformations = 1- Related to the motion of the center of mass- Zero due to momentum conservation
Connection with IBM: M. Macek et al., Phys. Rev. C 75, 064318 (2007)
3a. Geometric collective model
Zoom into the sea of levels
Dependence on the classicality parameter
E
<L2>
Dependence of the Brody parameter on energy
3a. Geometric collective model
Selected squared wave functions:
E
Peres operators & Wavefunctions
<L2>
<VB>
2D
Peres invariant classically
Poincaré sectionE = 0.2
3a. Geometric collective model
Classical and quantum measures - comparison Classical
measure
Quantum measure (Brody)
B = 0.24 B = 1.09
3a. Geometric collective model
Integrable case: = 2 expected
3.0 - 1.92x
6.0 - 1.93x
Shortest periodic classical orbit
Universal region
(averaged over 4 successive sets of 8192 levels, starting from level 8000)
(512 successive sets of 64 levels)
2.0 - 1.94x
log<S>
log f
1/f noise
Correlations we are interested in
Averaging of smaller intervals
3a. Geometric collective model
Mixed dynamics A = 0.25
reg
ula
rity
freg
- 11 -
E
Calculation of :Each point –
averaging over 32 successive sets of
64 levels in an energy window
1/f noise
3a. Geometric collective model
Interacting Boson Model
3b. Interacting boson model
IBM Hamiltonian
s-bosons (l=0) d-bosons (l=2)
- Valence nucleon pairs with l = 0, 2- quanta of quadrupole collective excitations
Symmetry
U(6) with 36 generatorstotal number of bosons is conserved
Dynamical symmetries (group chains)
The most general Hamiltonian (constructed from Casimir invariants of the subgoups)
vibrational
-unstable
rotational
nuclei
3b. Interacting boson model
SO(3) – total angular momentum L is conserved
U(5)SU(3)
SO(6)
0 0
1Arc of regularity
a – scaling parameter
Invariant of SO(5) (seniority)
Consistent-Q Hamiltonian
integrable casesClassical limit
via coherent states
F. Iachello, A. Arima, The Interacting Boson Model (Cambridge University Press, Cambridge, 1987)
quadrupole operator
d-boson number operator
3b. Interacting boson model
Shape phase transition
U(5)SU(3)
SO(6)
0 0
1
Casten triangle
a – scaling parameter
Invariant of SO(5) (seniority)
Consistent-Q Hamiltonian
integrable cases
3 independent
Peres operators
quadrupole operator
d-boson number operator
3b. Interacting boson model
Regular lattices in integrable case
3ˆ.ˆ SUQQ
dn̂v
- even the operators non-commuting with Casimirs of U(5) create regular lattices !
40
-40
-2020
10
30 -10
-30
0
-40
-20
-10
-30
0
0
3ˆ.ˆ SUQQ
6ˆ.ˆ OQQ
dn̂
L = 0
commuting non-commuting
U(5)
limit
N = 40
3b. Interacting boson model
Different invariants
= 0.5
N = 40
U(5)
SU(3)
O(5)
Arc of regularityArc of regularity
classical regularity
M. Macek, J. Dobeš, P. Cejnar, Phys. Rev. C 80, 014319 (2009)
3b. Interacting boson model
Different invariants
= 0.5
N = 40
U(5)
SU(3)
O(5)
Arc of regularityArc of regularity
classical regularity
Correspondence with GCM
<L2>
M. Macek, J. Dobeš, P. Cejnar, Phys. Rev. C 80, 014319 (2009)
3b. Interacting boson model
High-lying rotational bands
dn̂
N = 30L = 0
η = 0.5, χ= -1.04 (arc of regularity)
3ˆ.ˆ SUQQdn̂
3b. Interacting boson model
E
η = 0.5, χ= -1.04 (arc of regularity)
3ˆ.ˆ SUQQdn̂
High-lying rotational bands
3b. Interacting boson model
N = 30L = 0,2
E
η = 0.5, χ= -1.04 (arc of regularity)
3ˆ.ˆ SUQQdn̂
High-lying rotational bands
3b. Interacting boson model
N = 30L = 0,2,4
E
3ˆ.ˆ SUQQ
η = 0.5, χ= -1.04 (arc of regularity)
dn̂
High-lying rotational bands
3b. Interacting boson model
N = 30L = 0,2,4,6
Regular areas:Adiabatic separation of the intrinsic and collective motion
E
Numerical evidence of the rotational bands
Pearson correlation coefficient
=10/3 for rotational band
Classical fraction of regularity
M. Macek, J. Dobeš, P. Cejnar, Phys. Rev. C 81, 014318 (2010)
M. Macek, J. Dobeš, P. Stránský, P. Cejnar, Phys. Rev. Lett. 105, 072503 (2010)
3b. Interacting boson model
Components of eigenvectors in SU(3) basis
RB Appears naturally in the SU(3) basis
indices labeling the intrinsic , excitations (SU(3) basis states)
low-lying band highly excited band
Non-rotational sequence of states
3b. Interacting boson model
Quasidynamical symmetryThe characteristic features of a dynamical symmetry (the existence of the rotational bands here) survive despite the dynamical symmetry is broken
li – i-th eigenstate with angular momentum l
Summary1. Peres lattices
• Allow visualising quantum chaos• Capable of distinguishing between chaotic and
regular parts of the spectra• Freedom in choosing Peres operator
2. 1/f Noise• Effective method to introduce a measure of
chaos using long-range correlations in quantum spectra
3. Geometrical Collective Model• Complex behavior encoded in simple equations
(order-chaos-order transition)• Possibility of studying manifestations of both
classical and quantum chaos and their relation• Good classical-quantum correspondence
found even in the mixed dynamics regime
4. Interacting boson model• Peres operators come naturally from the
Casimirs of the dynamical symmetries groups• Evidence of connection between chaoticity
and separation of collective and intrinsic motions