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We extend Katok’s result on ‘the approximation of hyperbolic measures by horseshoes’ to Banach cocycles. More precisely, let f be a
$C^r(r>1)$
diffeomorphism of a compact Riemannian manifold M, preserving an ergodic hyperbolic measure
$\mu $
with positive entropy, and let
$\mathcal {A}$
be a Hölder continuous cocycle of bounded linear operators acting on a Banach space
$\mathfrak {X}$
. We prove that there is a sequence of horseshoes for f and dominated splittings for
$\mathcal {A}$
on the horseshoes, such that not only the measure theoretic entropy of f but also the Lyapunov exponents of
$\mathcal {A}$
with respect to
$\mu $
can be approximated by the topological entropy of f and the Lyapunov exponents of
$\mathcal {A}$
on the horseshoes, respectively. As an application, we show the continuity of sub-additive topological pressure for Banach cocycles.
Much research shows that the ratings that judges assign to the same wine are uncertain. And while the ratings may be independent, research also shows that they are not identically distributed. Thus, an acute difficulty in ratings-related research and in calculating consensus among judges is that each rating is one observation drawn from a latent distribution that is wine- and judge-specific. What can be deduced about the shape of a latent distribution from one observation? A simple maximum entropy estimator is proposed to describe the distribution of a rating observed. The estimator can express the implications of zero, one, a few blind replicates, and many observations. Several tests of the estimator show that results are consistent with the results of experiments with blind replicates and that results are more accurate than results based on observed ratings alone.
Physically based approaches to hydraulic geometry relations for width, depth, velocity, and slope require equations of continuity of water, roughness, and sediment transport. Different methods have been employed for different expressions of roughness and sediment transport. Without delving into their underlying theories, this chapter briefly outlines these expressions as they will be invoked in subsequent chapters. Also, unit stream power, stream power as well as entropy have been employed, which are also briefly discussed.
The structure of equilibrium thermodynamics, in harmony with statistical mechanics, does not contain a time asymmetry, except when it is trivially supplemented with one.
The two major questions posed by this chapter are: What is life and how do we define and identify it? How did life originate? It discusses different definitions of life and the role of entropy as a constraint. It discusses some forms that may or may not meet differing definitions of life (e.g. prions, viruses). The various hypotheses, studies, and discoveries pertaining to the origins of life are explored, including the Miller–Urey experiment, the Murcheson meteorite, and more recent NASA experiments relating to the potential origins of DNA and complex proteins. It also discusses the conditions on Earth during the origins of life, and presents the current hypotheses for the origins of water on this planet. It also reviews the candidates for the earliest life on Earth discovered in the fossil record, and explores just how we would identify the oldest life.
In this work, we study the entropies of subsystems of shifts of finite type (SFTs) and sofic shifts on countable amenable groups. We prove that for any countable amenable group G, if X is a G-SFT with positive topological entropy
$h(X)> 0$
, then the entropies of the SFT subsystems of X are dense in the interval
$[0, h(X)]$
. In fact, we prove a ‘relative’ version of the same result: if X is a G-SFT and
$Y \subset X$
is a subshift such that
$h(Y) < h(X)$
, then the entropies of the SFTs Z for which
$Y \subset Z \subset X$
are dense in
$[h(Y), h(X)]$
. We also establish analogous results for sofic G-shifts.
At the microscale, the motion of atoms and molecules composing matter is governed by Hamiltonian dynamics. For classical systems, this motion is described as trajectories in the phase space of the positions and momenta of the particles. Different equilibrium and nonequilibrium statistical ensembles can be introduced, each associated with some probability distribution, which is a solution of Liouville’s equation. The BBGKY hierarchy of equations is obtained for the multiparticle distribution functions. The presentation includes the properties of ergodicity and dynamical mixing, the Pollicott–Ruelle resonances, microreversibility, and the nonequilibrium breaking of time-reversal symmetry at the statistical level of description. The concept of entropy is introduced by coarse graining. Linear response theory is developed within the classical framework, leading to the Onsager–Casimir reciprocal relations and the fluctuation–dissipation theorem. The projection-operator methods are summarized.
At the macroscale, thermodynamics rules the balances of energy and entropy. In nonisolated systems, the entropy changes due to the contributions from the internal entropy production, which is always nonnegative according to the second law, and the exchange of entropy with the environment. The entropy production is equal to zero at equilibrium and positive out of equilibrium. Thermodynamics can be formulated either locally for continuous media or globally for systems in contact with several reservoirs. Accordingly, the entropy production is expressed in terms of either the local or the global affinities and currents, the affinities being the thermodynamic forces driving the system away from equilibrium. Depending on the boundary and initial conditions, the system can undergo relaxation towards equilibrium or nonequilibrium stationary or time-dependent macrostates. As examples, thermodynamics is applied to diffusion, electric circuits, reaction networks, and engines.
For a
$C^{1+\alpha }$
diffeomorphism f of a compact smooth manifold, we give a necessary and sufficient condition that guarantees that if the set of hyperbolic Lyapunov–Perron regular points has positive volume, then f preserves a smooth measure. We use recent results on symbolic coding of
$\chi $
-non-uniformly hyperbolic sets and results concerning the existence of SRB measures for them.
Chapter 3 derives the gap equation and determines the critical transition temperature as well as the zero-temperature energy gap as a function of coupling constant for d-wave superconductors. The energy dependence of the density of states and its effects on the temperature dependence of the gap function, entropy and other thermodynamic quantities are also discussed. Low energy nodal excitations lead to characteristic power-law behaviors in the specific heat or other thermodynamic response functions of d-wave superconductors at low temperatures, in contrast to the activated behaviors in s-wave superconductors. The probability density current and charge density current operators of d-wave quasiparticles, together with the gap operators in the continuum limit, are derived and discussed with the BdG framework.
Chapter 8 studies the many-impurity scattering effects in d-wave superconductors, particularly in the unitary or Born scattering limit. The impurity corrections to self-energy, density of states, superconducting critical temperature, entropy and specific heat are derived and compared with measurement data for high-Tc superconductors.
Let
$(X_k)_{k\geq 0}$
be a stationary and ergodic process with joint distribution
$\mu $
, where the random variables
$X_k$
take values in a finite set
$\mathcal {A}$
. Let
$R_n$
be the first time this process repeats its first n symbols of output. It is well known that
$({1}/{n})\log R_n$
converges almost surely to the entropy of the process. Refined properties of
$R_n$
(large deviations, multifractality, etc) are encoded in the return-time
$L^q$
-spectrum defined as
provided the limit exists. We consider the case where
$(X_k)_{k\geq 0}$
is distributed according to the equilibrium state of a potential with summable variation, and we prove that
where
$P((1-q)\varphi )$
is the topological pressure of
$(1-q)\varphi $
, the supremum is taken over all shift-invariant measures, and
$q_\varphi ^*$
is the unique solution of
$P((1-q)\varphi ) =\sup _\eta \int \varphi \,d\eta $
. Unexpectedly, this spectrum does not coincide with the
$L^q$
-spectrum of
$\mu _\varphi $
, which is
$P((1-q)\varphi )$
, and it does not coincide with the waiting-time
$L^q$
-spectrum in general. In fact, the return-time
$L^q$
-spectrum coincides with the waiting-time
$L^q$
-spectrum if and only if the equilibrium state of
$\varphi $
is the measure of maximal entropy. As a by-product, we also improve the large deviation asymptotics of
$({1}/{n})\log R_n$
.
We present several applications of the weak specification property and certain topological Markov properties, recently introduced by Barbieri, García-Ramos, and Li [Markovian properties of continuous group actions: algebraic actions, entropy and the homoclinic group. Adv. Math.397 (2022), 52], and implied by the pseudo-orbit tracing property, for general expansive group actions on compact spaces. First we show that any expansive action of a countable amenable group on a compact metrizable space satisfying the weak specification and strong topological Markov properties satisfies the Moore property, that is, every surjective endomorphism of such dynamical system is pre-injective. This together with an earlier result of Li (where the strong topological Markov property is not needed) of the Myhill property [Garden of Eden and specification. Ergod. Th. & Dynam. Sys.39 (2019), 3075–3088], which we also re-prove here, establishes the Garden of Eden theorem for all expansive actions of countable amenable groups on compact metrizable spaces satisfying the weak specification and strong topological Markov properties. We hint how to easily generalize this result even for uncountable amenable groups and general compact, not necessarily metrizable, spaces. Second, we generalize the recent result of Cohen [The large scale geometry of strongly aperiodic subshifts of finite type. Adv. Math.308 (2017), 599–626] that any subshift of finite type of a finitely generated group having at least two ends has weakly periodic points. We show that every expansive action of such a group having a certain Markov topological property, again implied by the pseudo-orbit tracing property, has a weakly periodic point. If it has additionally the weak specification property, the set of such points is dense.
We show that the complete positive entropy (CPE) class
$\alpha $
of Barbieri and García-Ramos contains a one-dimensional subshift for all countable ordinals
$\alpha $
, that is, the process of alternating topological and transitive closure on the entropy pairs relation of a subshift can end on an arbitrary ordinal. This is the composition of three constructions. We first realize every ordinal as the length of an abstract ‘close-up’ process on a countable compact space. Next, we realize any abstract process on a compact zero-dimensional metrizable space as the process started from a shift-invariant relation on a subshift, the crucial construction being the implementation of every compact metrizable zero-dimensional space as an open invariant quotient of a subshift. Finally, we realize any shift-invariant relation E on a subshift X as the entropy pair relation of a supershift
$Y \supset X$
, and under strong technical assumptions, we can make the CPE process on Y end on the same ordinal as the close-up process of E.
Anti-evolutionists sometimes use principles of thermodynamics in making their case. Though thermodynamics is normally considered a branch of physics, it has a strongly mathematical character that justifies its inclusion in this book. We discuss the basics of thermodynamics and statistical mechanics, and then explain why the anti-evolutionist version is such a caricature.
In this chapter, spacetime is identified as the empirical realm, to be understood in a relational sense. The spacetime construct emerges from the quantum substratum by way of actualized transactions, which establish spacetime events and their structural connections. This process is discussed in terms of causal set theory. The quantum substratum constitutes the reference for “absolute motion,” and rest-mass systems in the substratum define inertial frames. The transactional process breaks time symmetry, thus establishing an arrow of time and shedding light on the Second Law of Thermodynamics. Implications for free will are also discussed.
In this text, we provide a fully rigorous and complete proof of E.H. Lieb’s statement that (topological) entropy of square ice (or six-vertex model, XXZ spin chain for anisotropy parameter $\Delta =1/2$) is equal to $\tfrac 32\log _{2} (4/3)$.
The Halphen type B (Hal-B) frequency distribution has been employed for frequency analyses of hydrometeorological and hydrological extremes. This chapter derives this distribution using entropy theory and discusses the estimation of its parameters with the use of the constraints used for their derivation. The distribution i+L13s tested using entropy and the methods of moments and maximum likelihood estimation.