This document summarizes research on quantum chaos, including the principle of uniform semiclassical condensation of Wigner functions, spectral statistics in mixed systems, and dynamical localization of chaotic eigenstates. It discusses how in the semiclassical limit, Wigner functions condense uniformly on classical invariant components. For mixed systems, the spectrum can be seen as a superposition of regular and chaotic level sequences. Localization effects can be observed if the Heisenberg time is shorter than the classical diffusion time. The document presents an analytical formula called BRB that describes the transition between Poisson and random matrix statistics. An example is given of applying this to analyze the level spacing distribution for a billiard system.
Disturbo da gioco d’azzardo: aspetti biopsicosociali e normative vigentiNicola Piccinini
Quanto è vera ancora oggi questa frase! E’ tanto più vera quanto più ci avviciniamo dal gioco ricreazionale a quello patologico. Non più vizio, ma mera malattia nella società post-moderna, dove l’alienazione è l’effetto collaterale tra i più disastrosi del consumismo che crea bisogni continui di riempire i vuoti creati dal desiderio di beni da consumare arrivando alla “coazione a ripetere”: dallo “star bene con” allo “star male senza”, vere e proprie “distorsioni dello stile cognitivo”.
Nell’ultima edizione del DSM V, il Disturbo da Gioco d’Azzardo (Gambling Disorder) assume una sua specifica posizione: da patologia del controllo degli impulsi gli viene riconosciuto lo status di dipendenza comportamentale. Questo è un importante cambiamento epistemologico che evidenzia le analogie, confermate dall’evidenze scientifiche, tra il gambling e le dipendenze chimiche. La questione ha rilevanza clinica in quanto autorizza i professionisti del settore ad applicare al gambling patologico strumenti di assessment e terapeutici propri dei programmi per l'addiction supportati anche dal Decreto- Balduzzi che con la legge 189/2012 (c.d. Decreto Balduzzi) attua importanti interventi in materia di tutela della salute ed organizzazione del Servizio Sanitario Nazionale. Vengono varate, per la prima volta in Italia, norme a favore della cura e della prevenzione del gioco d’azzardo patologico. Il primo punto qualificante del “decreto Balduzzi” su questa materia è costituito dal riconoscimento del gioco d’azzardo patologico come una malattia inserita nell’elenco dei livelli essenziali di assistenza (LEA).
Disturbo da gioco d’azzardo: aspetti biopsicosociali e normative vigentiNicola Piccinini
Quanto è vera ancora oggi questa frase! E’ tanto più vera quanto più ci avviciniamo dal gioco ricreazionale a quello patologico. Non più vizio, ma mera malattia nella società post-moderna, dove l’alienazione è l’effetto collaterale tra i più disastrosi del consumismo che crea bisogni continui di riempire i vuoti creati dal desiderio di beni da consumare arrivando alla “coazione a ripetere”: dallo “star bene con” allo “star male senza”, vere e proprie “distorsioni dello stile cognitivo”.
Nell’ultima edizione del DSM V, il Disturbo da Gioco d’Azzardo (Gambling Disorder) assume una sua specifica posizione: da patologia del controllo degli impulsi gli viene riconosciuto lo status di dipendenza comportamentale. Questo è un importante cambiamento epistemologico che evidenzia le analogie, confermate dall’evidenze scientifiche, tra il gambling e le dipendenze chimiche. La questione ha rilevanza clinica in quanto autorizza i professionisti del settore ad applicare al gambling patologico strumenti di assessment e terapeutici propri dei programmi per l'addiction supportati anche dal Decreto- Balduzzi che con la legge 189/2012 (c.d. Decreto Balduzzi) attua importanti interventi in materia di tutela della salute ed organizzazione del Servizio Sanitario Nazionale. Vengono varate, per la prima volta in Italia, norme a favore della cura e della prevenzione del gioco d’azzardo patologico. Il primo punto qualificante del “decreto Balduzzi” su questa materia è costituito dal riconoscimento del gioco d’azzardo patologico come una malattia inserita nell’elenco dei livelli essenziali di assistenza (LEA).
Birkhoff coordinates for the Toda Lattice in the limit of infinitely many par...Alberto Maspero
We study the Birkhoff coordinates (Cartesian action angle coordinates) of the Toda lattice with periodic boundary condition in the limit where the number N of the particles tends to infinity. We prove that the transformation introducing such coordinates maps analytically a complex ball of radius R/Nα (in discrete Sobolev-analytic norms) into a ball of radius R′/Nα (with R,R′>0 independent of N) if and only if α≥2. Then we consider the problem of equipartition of energy in the spirit of Fermi-Pasta-Ulam. We deduce that corresponding to initial data of size R/N2, 0<R≪1, and with only the first Fourier mode excited, the energy remains forever in a packet of Fourier modes exponentially decreasing with the wave number. Finally we consider the original FPU model and prove that energy remains localized in a similar packet of Fourier modes for times one order of magnitude longer than those covered by previous results which is the time of formation of the packet. The proof of the theorem on Birkhoff coordinates is based on a new quantitative version of a Vey type theorem by Kuksin and Perelman which could be interesting in itself.
kinks and cusps in the transition dynamics of a bloch statejiang-min zhang
We discuss the transition dynamics of a Bloch state in a 1D tight binding chain, under two scenarios, namely, weak periodical driving [1] and sudden quench [2]. In the former case, the survival probability of the initial Bloch state shows kinks periodically; it is a piece-wise linear function of time. In the latter, the survival probability (Loschmidt echo in this case) shows cusps periodically; it is a piece-wise quadratic function of time. Kinks in the former case are a perturbative effect, while cusps in the latter are a non-perturbative effect. The kinks and cusps are reminiscent of the so-called dynamical phase transtion termed by Heyl et al. [3].
[1] J. M. Zhang and M. Haque, Nonsmooth and level-resolved dynamics illustrated with the tight binding model, arXiv:1404.4280.
[2] J. M. Zhang and H. T. Yang, Cusps in the quenched dynamics of a bloch state, arXiv:1601.03569.
[3] M. Heyl, A. Polkovnikov, and S. Kehrein, Dynamical quantum phase transitions in the transverse-field Ising model, Phys. Rev. Lett. 110, 135704 (2013).
We research behavior and sharp bounds for the zeros of infinite sequences of polynomials orthogonal with respect to a Geronimus perturbation of a positive Borel measure on the real line.
UCSD NANO 266 Quantum Mechanical Modelling of Materials and Nanostructures is a graduate class that provides students with a highly practical introduction to the application of first principles quantum mechanical simulations to model, understand and predict the properties of materials and nano-structures. The syllabus includes: a brief introduction to quantum mechanics and the Hartree-Fock and density functional theory (DFT) formulations; practical simulation considerations such as convergence, selection of the appropriate functional and parameters; interpretation of the results from simulations, including the limits of accuracy of each method. Several lab sessions provide students with hands-on experience in the conduct of simulations. A key aspect of the course is in the use of programming to facilitate calculations and analysis.
How to find a cheap surrogate to approximate Bayesian Update Formula and to a...Alexander Litvinenko
We suggest the new vision for classical Bayesian Update formula. We expand all ingredients in Polynomial Chaos Expansion and write out a new formula for Bayesian* update of PCE coefficients. This formula is derived from Minimum Mean Square Estimation. One starts with prior PCE, take measurements into account, and obtain posterior PCE coefficients, without any MCMC sampling.
Birkhoff coordinates for the Toda Lattice in the limit of infinitely many par...Alberto Maspero
We study the Birkhoff coordinates (Cartesian action angle coordinates) of the Toda lattice with periodic boundary condition in the limit where the number N of the particles tends to infinity. We prove that the transformation introducing such coordinates maps analytically a complex ball of radius R/Nα (in discrete Sobolev-analytic norms) into a ball of radius R′/Nα (with R,R′>0 independent of N) if and only if α≥2. Then we consider the problem of equipartition of energy in the spirit of Fermi-Pasta-Ulam. We deduce that corresponding to initial data of size R/N2, 0<R≪1, and with only the first Fourier mode excited, the energy remains forever in a packet of Fourier modes exponentially decreasing with the wave number. Finally we consider the original FPU model and prove that energy remains localized in a similar packet of Fourier modes for times one order of magnitude longer than those covered by previous results which is the time of formation of the packet. The proof of the theorem on Birkhoff coordinates is based on a new quantitative version of a Vey type theorem by Kuksin and Perelman which could be interesting in itself.
kinks and cusps in the transition dynamics of a bloch statejiang-min zhang
We discuss the transition dynamics of a Bloch state in a 1D tight binding chain, under two scenarios, namely, weak periodical driving [1] and sudden quench [2]. In the former case, the survival probability of the initial Bloch state shows kinks periodically; it is a piece-wise linear function of time. In the latter, the survival probability (Loschmidt echo in this case) shows cusps periodically; it is a piece-wise quadratic function of time. Kinks in the former case are a perturbative effect, while cusps in the latter are a non-perturbative effect. The kinks and cusps are reminiscent of the so-called dynamical phase transtion termed by Heyl et al. [3].
[1] J. M. Zhang and M. Haque, Nonsmooth and level-resolved dynamics illustrated with the tight binding model, arXiv:1404.4280.
[2] J. M. Zhang and H. T. Yang, Cusps in the quenched dynamics of a bloch state, arXiv:1601.03569.
[3] M. Heyl, A. Polkovnikov, and S. Kehrein, Dynamical quantum phase transitions in the transverse-field Ising model, Phys. Rev. Lett. 110, 135704 (2013).
We research behavior and sharp bounds for the zeros of infinite sequences of polynomials orthogonal with respect to a Geronimus perturbation of a positive Borel measure on the real line.
UCSD NANO 266 Quantum Mechanical Modelling of Materials and Nanostructures is a graduate class that provides students with a highly practical introduction to the application of first principles quantum mechanical simulations to model, understand and predict the properties of materials and nano-structures. The syllabus includes: a brief introduction to quantum mechanics and the Hartree-Fock and density functional theory (DFT) formulations; practical simulation considerations such as convergence, selection of the appropriate functional and parameters; interpretation of the results from simulations, including the limits of accuracy of each method. Several lab sessions provide students with hands-on experience in the conduct of simulations. A key aspect of the course is in the use of programming to facilitate calculations and analysis.
How to find a cheap surrogate to approximate Bayesian Update Formula and to a...Alexander Litvinenko
We suggest the new vision for classical Bayesian Update formula. We expand all ingredients in Polynomial Chaos Expansion and write out a new formula for Bayesian* update of PCE coefficients. This formula is derived from Minimum Mean Square Estimation. One starts with prior PCE, take measurements into account, and obtain posterior PCE coefficients, without any MCMC sampling.
Similar to Quantum chaos of generic systems - Marko Robnik (20)
Slide 1: Title Slide
Extrachromosomal Inheritance
Slide 2: Introduction to Extrachromosomal Inheritance
Definition: Extrachromosomal inheritance refers to the transmission of genetic material that is not found within the nucleus.
Key Components: Involves genes located in mitochondria, chloroplasts, and plasmids.
Slide 3: Mitochondrial Inheritance
Mitochondria: Organelles responsible for energy production.
Mitochondrial DNA (mtDNA): Circular DNA molecule found in mitochondria.
Inheritance Pattern: Maternally inherited, meaning it is passed from mothers to all their offspring.
Diseases: Examples include Leber’s hereditary optic neuropathy (LHON) and mitochondrial myopathy.
Slide 4: Chloroplast Inheritance
Chloroplasts: Organelles responsible for photosynthesis in plants.
Chloroplast DNA (cpDNA): Circular DNA molecule found in chloroplasts.
Inheritance Pattern: Often maternally inherited in most plants, but can vary in some species.
Examples: Variegation in plants, where leaf color patterns are determined by chloroplast DNA.
Slide 5: Plasmid Inheritance
Plasmids: Small, circular DNA molecules found in bacteria and some eukaryotes.
Features: Can carry antibiotic resistance genes and can be transferred between cells through processes like conjugation.
Significance: Important in biotechnology for gene cloning and genetic engineering.
Slide 6: Mechanisms of Extrachromosomal Inheritance
Non-Mendelian Patterns: Do not follow Mendel’s laws of inheritance.
Cytoplasmic Segregation: During cell division, organelles like mitochondria and chloroplasts are randomly distributed to daughter cells.
Heteroplasmy: Presence of more than one type of organellar genome within a cell, leading to variation in expression.
Slide 7: Examples of Extrachromosomal Inheritance
Four O’clock Plant (Mirabilis jalapa): Shows variegated leaves due to different cpDNA in leaf cells.
Petite Mutants in Yeast: Result from mutations in mitochondrial DNA affecting respiration.
Slide 8: Importance of Extrachromosomal Inheritance
Evolution: Provides insight into the evolution of eukaryotic cells.
Medicine: Understanding mitochondrial inheritance helps in diagnosing and treating mitochondrial diseases.
Agriculture: Chloroplast inheritance can be used in plant breeding and genetic modification.
Slide 9: Recent Research and Advances
Gene Editing: Techniques like CRISPR-Cas9 are being used to edit mitochondrial and chloroplast DNA.
Therapies: Development of mitochondrial replacement therapy (MRT) for preventing mitochondrial diseases.
Slide 10: Conclusion
Summary: Extrachromosomal inheritance involves the transmission of genetic material outside the nucleus and plays a crucial role in genetics, medicine, and biotechnology.
Future Directions: Continued research and technological advancements hold promise for new treatments and applications.
Slide 11: Questions and Discussion
Invite Audience: Open the floor for any questions or further discussion on the topic.
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Earliest Galaxies in the JADES Origins Field: Luminosity Function and Cosmic ...Sérgio Sacani
We characterize the earliest galaxy population in the JADES Origins Field (JOF), the deepest
imaging field observed with JWST. We make use of the ancillary Hubble optical images (5 filters
spanning 0.4−0.9µm) and novel JWST images with 14 filters spanning 0.8−5µm, including 7 mediumband filters, and reaching total exposure times of up to 46 hours per filter. We combine all our data
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30.3-31.0 AB mag (5σ, r = 0.1” circular aperture) in individual filters. We measure photometric
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z = 11.5 − 15. These objects show compact half-light radii of R1/2 ∼ 50 − 200pc, stellar masses of
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Earliest Galaxies in the JADES Origins Field: Luminosity Function and Cosmic ...
Quantum chaos of generic systems - Marko Robnik
1. Center for Applied Mathematics and Theoretical Physics
University of Maribor • Maribor • Slovenia
www.camtp.uni-mb.si
Quantum chaos of generic systems
Marko Robnik
Let’s Face Complexity
New Bridges Between Physical and Social Sciences
Como, Italy, 4-8 September 2017
2. COLLABORATORS
Prof.Dr. Tomaˇz Prosen, former PhD student, now at University of Ljubljana
Prof.Dr. Baowen Li, former postdoc, now at National University of Singapore
Prof.Dr. Gregor Veble, former PhD student, now chief aerodynamicist at
Joby Aviation
Dr. Gregor Vidmar, former PhD student, now at University of Ljubljana
Prof. Dr. Hans-J¨urgen St¨ockmann, University of Marburg, Germany
Dr. Benjamin Batisti´c, former PhD student, now postdoc at CAMTP
Dr. Thanos Manos, former postdoc, now postdoc at J¨ulich, Germany
Mr. ˇCrt Lozej, PhD student, CAMTP
3. CONTENTS
0. Motivation by example: Quantum billiards: Helmholtz equation
1. Introduction: Universality classes of spectral fluctuations
2. Principle of Uniform Semiclassical Condensation (PUSC) of Wigner f.
3. Mixed type systems in the semiclassical limit:
3.1 Spectral statistics of regular and chaotic level sequences
3.2 Separation of regular and chaotic eigenstates
4. Quantum localization of chaotic eigenstates
5. Discussion and conclusions
6. References
4. Motivation by example
Two-dimensional classical billiards:
A point particle moving freely inside a two-dimensional domain
with specular reflection on the boundary upon the collision:
Energy (and the speed) of the particle is conserved.
A particular example of the billiard boundary shape as a model system:
Complex map: z → w, |z| = 1
w = z + λz2
,
6. Motivation by example
Two-dimensional quantum billiards
Helmholtz equation with Dirichlet boundary conditions
∂2
ψ
∂x2 + ∂2
ψ
∂y2 + Eψ = 0
with ψ = 0 on the boundary
7.
8.
9.
10.
11. Example of mixed type system: Hydrogen atom in strong magnetic field
H =
p2
2me
−
e2
r
+
eLz
2mec
|B| +
e2
B2
8mec2
ρ2
B = magnetic field strength vector pointing in z-direction
r = x2 + y2 + z2 = spherical radius, ρ = x2 + y2 = axial radius
Lz = z-component of angular momentum = conserved quantity
Characteristic field strength: B0 =
m2
ee3
c
¯h2 = 2.35 × 109
Gauss = 2.35 × 105
Tesla
Rough qualitative criterion for global chaos: magnetic force ≈ Coulomb force
(Wunner et al 1978+; Wintgen et al 1987+; Hasegawa, R. and Wunner 1989,
Friedrich and Wintgen 1989; classical and quantum chaos: R. 1980+)
12.
13.
14. spectral unfolding procedure: transform the energy spectrum to unit mean
level spacing (or density)
After such spectral unfolding procedure we are describing the spectral statistical
properties, that is statistical properties of the eigenvalues.
Two are most important:
Level spacing distribution: P(S)
P(S)dS = Probability that a nearest level spacing S is within (S, S + dS)
E(k,L) = probability of having precisely k levels on an interval of length L
Important special case is the gap probability E(0, L) = E(L) of having no levels on
an interval of length L, and is related to the level spacing distribution:
P(S) = d2
E(S)
dS2
15. The Gaussian Random Matrix Theory
P({Hij})d{Hij} = probability of the matrix elements {Hij} inside the volume
element d{Hij}
We are looking for the statistical properties of the eigenvalues
A1 P({Hij}) = P(H) is invariant against the group transformations, which preserve
the structure of the matrix ensemble:
orthogonal transformations for the real symmetric matrices: GOE
unitary transformations for the complex Hermitian matrices: GUE
It follows that P(H) must be a function of the invariants of H
A2 The matrix elements are statistically independently distributed:
P(H11, . . . , HNN) = P(H11) . . . P(HNN)
It follows from these two assumptions that the distribution P(Hij) must be Gaussian:
There is no free parameter: Universality
16. 2D GOE and GUE of random matrices:
Quite generally, for a Hermitian matrix
x y + iz
y − iz −x
with x, y, z real
the eigenvalue λ = ± x2 + y2 + z2 and level spacing
S = λ1 − λ2 = 2 x2 + y2 + z2
The level spacing distribution is
P(S) =
R3
dx dy dz gx(x)gy(y)gz(z)δ(S − 2 x2 + y2 + z2) (1)
which is equivalent to 2D GOE/GUE when gx(u) = gy(u) = gz(u) = 1
σ
√
π
exp(−u2
σ2)
and after normalization to < S >= 1
• 2D GUE P(S) = 32S2
π2 exp(−4S2
π ) Quadratic level repulsion
• 2D GOE gz(u) = δ(u) and P(S) = πS
2 exp(−πS2
4 ) Linear level repulsion
There is no free parameter: Universality
17.
18. The Main Assertion of Stationary Quantum Chaos
(Casati, Valz-Gries, Guarneri 1980; Bohigas, Giannoni, Schmit 1984; Percival 1973)
(A1) If the system is classically integrable: Poissonian spectral statistics
(A2) If classically fully chaotic (ergodic): Random Matrix Theory (RMT) applies
• If there is an antiunitary symmetry, we have GOE statistics
• If there is no antiunitary symmetry, we have GUE statistics
(A3) If of the mixed type, in the deep semiclassical limit: we have no spectral
correlations: the spectrum is a statistically independent superposition of regular
and chaotic level sequences:
E(k, L) =
k1+k2+...+km=k
j=m
j=1
Ej(kj, µjL) (2)
µj= relative fraction of phase space volume = relative density of corresponding
quantum levels. j = 1 is the Poissonian, j ≥ 2 chaotic, and µ1 + µ2 + ... + µm = 1
19. According to our theory, for a two-component system, j = 1, 2, we have (Berry and
Robnik 1984):
E(0, S) = E1(0, µ1S)E2(0, µ2S)
Poisson (regular) component: E1(0, S) = e−S
Chaotic (irregular) component: E2(0, S) = erfc
√
πS
2 (Wigner = 2D GOE)
E(0, S) = E1(0, µ1S)E2(0, µ2S) = e−µ1S
erfc(
√
πµ2S
2 ), where µ1 + µ2 = 1.
Then P(S) = level spacing distribution = d2
E(0,S)
dS2 and we obtain:
PBR(S) = e−µ1S
exp(−
πµ2
2S2
4 )(2µ1µ2 +
πµ3
2S
2 ) + µ2
1erfc(µ2
√
πS
2 )
(Berry and Robnik 1984)
This is a one parameter family of distribution functions with normalized total
probability < 1 >= 1 and mean level spacing < S >= 1, whilst the second moment
can be expressed in the closed form and is a function of µ1.
20.
21.
22. THE IMPORTANT SEMICLASSICAL CONDITION
The semiclassical condition for the random matrix theory to apply in the chaotic
eigenstates is that the Heisenberg time tH is larger than all classical transport times
tT of the system!
The Heisenberg time of any quantum system= tH = 2π¯h
∆E = 2π¯hρ(E)
∆E = 1/ρ(E) is the mean energy level spacing, ρ(E) is the mean level density
The quantum evolution follows the classical evolution including the chaotic diffusion
up to the Heisenberg time, at longer times the destructive interference sets in and
causes
the quantum or dynamical localization
Note: ρ(E) ∝ 1
(2π¯h)N → ∞ when ¯h → 0, and therefore eventually tH tT .
This observation applies to time-dependent and to time-independent systems.
23. We show the second moment p2
averaged over an ensemble of 106
initial
conditions uniformly distributed in the chaotic component on the interval
s ∈ [0, L/2] and p = 0.. We see that the saturation value of p2
is reached at about
NT = 105
collisions for λ = 0.15, NT = 103
collisions for λ = 0.20 and NT = 102
for
λ = 0.25. For λ = 0.15, according to the criterion at k = 2000 and k = 4000, we are
still in the regime where the dynamical localization is expected. On the other hand,
for λ = 0.20, 0.25 we expect extended states already at k < 2000.
24.
25. 2. Principle of Uniform Semiclassical Condensation (PUSC) of Wigner
functions of eigenstates (Percival 1973, Berry 1977, Shnirelman 1979, Voros 1979,
Robnik 1987-1998)
We study the structure of eigenstates in ”quantum phase space”: The Wigner
functions of eigenstates (they are real valued but not positive definite):
Definition: Wn(q, p) = 1
(2π¯h)N dN
X exp −i
¯hp.X ψn(q − X
2 )ψ∗
n(q + X
2 )
(P1) Wn(q, p)dN
p = |ψn(q)|2
(P2) Wn(q, p)dN
q = |φn(p)|2
(P3) Wn(q, p)dN
q dN
p = 1
(P4) (2π¯h)N
dN
q dN
pWn(q, p)Wm(q, p) = δnm
(P5) |Wn(q, p)| ≤ 1
(π¯h)N (Baker 1958)
(P6 = P4) W2
n(q, p)dN
q dN
p = 1
(2π¯h)N
(P7) ¯h → 0 : Wn(q, p) → (2π¯h)N
W2
n(q, p) > 0
26. In the semiclassical limit the Wigner functions condense on an element of phase
space of volume size (2π¯h)N
(elementary quantum Planck cell) and become positive
definite there.
Principle of Uniform Semiclassical Condensation (PUSC)
Wigner fun. Wn(q, p) condenses uniformly on a classically invariant component:
(C1) invariant N-torus (integrable or KAM): Wn(q, p) = 1
(2π)N δ (I(q, p) − In)
(C2) uniform on topologically transitive chaotic region:
Wn(q, p) = δ(En−H(q,p)) χω(q,p)
dNq dNp δ(En−H(q,p)) χω(q,p)
where χω(q, p) is the characteristic function on the chaotic component indexed by ω
(C3) ergodicity: microcanonical: Wn(q, p) = δ(En−H(q,p))
dNq dNp δ(En−H(q,p)
Important: Relative Liouville measure of the classical invariant component:
µ(ω) =
dN
q dN
p δ(En−H(q,p)) χω(q,p)
dNq dNp δ(En−H(q,p))
27. How good is this theory at sufficiently small effective ¯h?
28.
29. 4. Approach to describe the semiclassical transition regime
If we are not sufficiently deep in the semiclassical regime of sufficiently small effective
Planck constant ¯heff, which e.g. in billiards means not at sufficiently high energies,
we observe two new effects, which are the cause for the deviation from BR
statistics:
• Localization of eigenstates, due to the dynamical localization: The Wigner
functions are no longer uniformly spread over the classically available chaotic
component but are localized instead.
• Coupling due to tunneling between the semiclassical regular (R) and chaotic (C)
states
This effect typically disappears very quickly with increasing energy, due to the
exponential dependence on 1/¯heff.
30. Rough criterion for dynamical localization:
Heisenberg time tH = 2π¯h/(mean energy level spacing) = 2π¯h× (level density)
If the Heisenberg time tH is shorter than the classical diffusion time we observe the
localization, and extended (delocalized) states otherwise.
The Heisenberg time tH ∝ ¯h(1−N)
goes to infinity with ¯h → 0, therefore
asymptotically we always reach extended chaotic states and BR statistics.
But below the BR regime the effects of localization are observed, and can survive to
very high lying eigenstates, even up to one million above the ground state.
We shall illustrate the results in real billiard spectra.
31. Dynamically localized chaotic states are semiempirically well described by the
Brody level spacing distribution: (Izrailev 1988,1989, Prosen and Robnik1993/4)
PB(S) = C1Sβ
exp −C2Sβ+1
, FB(S) = 1 − WB(S) = exp −C2Sβ+1
,
where β ∈ [0, 1] and the two parameters C1 and C2 are determined by the two
normalizations < 1 >=< S >= 1, and are given by
C1 = (β + 1)C2, C2 = Γ β+2
β+1
β+1
with Γ(x) being the Gamma function. If we
have extended chaotic states β = 1 and RMT applies, whilst in the strongly localized
regime β = 0 and we have Poissonian statistics. The corresponding gap probability is
EB(S) =
1
(β + 1)Γ β+2
β+1
Q
1
β + 1
, Γ
β + 2
β + 1
S
β+1
Q(α, x) is the incomplete Gamma function: Q(α, x) =
∞
x
tα−1
e−t
dt.
32. The BRB theory: BR-Brody
(Prosen and Robnik 1993/1994, Batisti´c and Robnik 2010)
We have divided phase space µ1 + µ2 = 1 and localization β:
E(S) = Er(µ1S)Ec(µ2S) = exp(−µ1S)EBrody(µ2S)
and the level spacing distribution P(S) is:
P(S) =
d2
Er
dS2
Ec + 2
dEr
dS
dEc
dS
+ Er
d2
Ec
dS2
33. We study the billiard defined by the quadratic complex conformal mapping:
w(z) = z + λz2
of the unit circle |z| = 1 (introduced in R. 1983/1984).
We chose λ = 0.15, for which ρ1 = 0.175
We plot the level spacing distribution P(S)
34. The level spacing distribution for the billiard λ = 0.15, compared with the analytical
formula for BRB (red full line) with parameter values ρ1 = 0.183, β = 0.465 and
σ = 0. The dashed red curve close to the full red line is BRB with classical
ρ1 = 0.175 is not visible, as it overlaps completely with the quantum case
ρ1 = 0.183. The dashed curve far away from the red full line is just the BR curve
with the classical ρ1 = 0.175. The Poisson and GOE curves (dotted) are shown for
comparison. The agreement of the numerical spectra with BRB is perfect. In the
histogram we have 650000 objects, and the statistical significance is extremely large.
35. Discussion and conclusions
• The Principle of Uniform Semiclassical Condensation of Wigner functions of
eigenstates leads to the idea that in the sufficiently deep semiclassical limit the
spectrum of a mixed type system can be described as a statistically independent
superposition of regular and chaotic level sequences.
• As a result of that the E(k, L) probabilities factorize and the level spacings and
other statistics can be calculated in a closed form.
• At lower energies we see quantum or dynamical localization.
• The level spacing distribution of localized chaotic eigenstates is excellently
described by the Brody distribution with β ∈ [0, 1].
• In the mixed type systems regular and chaotic eigenstates can be separated: the
regular obey Poisson, the localized chaotic states obey the Brody.
• The Brody level repulsion exponent β is a function of the localization measure A.
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