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In this short chapter, we show that the edge-kstar model exhibits many of the properties of the edge-2star model. In particular: all entropy maximizers are multipodal with a uniform bound on the number of defining parameters; there is a single bipodal phase along the lower boundary of the phase space; near the top of the phase space there is a phase transition between cliquelike and anticliquelike graphs, with two optimal graphons on the curve dividing these regions. We also show that there is a bipodal phase in a model where we constrain an arbitrary positive linear combination of kstar densities. As we will see in Chapter 7, every edge-H model (where H is a fixed graph) is well approximated by an edge-(linear combination of kstars) model. The estimates of this chapter are at the core of the proof of Theorem 7.11, proving the existence of a bipodal phase for all edge-H models.
In this short chapter, we establish some basic facts about the edge-triangle model. We review Pikhurko and Razborov’s results about the geography of the phase space of possible values of pairs of the edge and triangle densities, the so-called Razborov triangle. We derive the unique entropy-maximizing graphon at each point on the boundary, and prove that there is a phase transition across the so-called Erdős–Rényi curve in the middle of the phase space. We compute the optimal graphon along a certain line segment that is disjoint from the Erdős–Rényi curve, answering an old question of Chatterjee and Diaconis. Along the way, we develop several proof techniques that will be repeated throughout the book, in particular the Method of Saturated Inequalities and the Method of Competing Inequalities.
In this chapter, the details of atmospheric phase transitions, nucleation, and cloud droplet formation are discussed. Some phase transitions require a nucleation process, for example, the freezing of liquids, for example ice nucleation. Other phase transitions, such as those involved in cloud droplet formation, do not require a nucleation process because cloud droplets form on water-soluble aerosol particles such as salts. Such aerosol particles often exist in the atmosphere as aqueous solution droplets because they take up water and develop a liquid phase through hygroscopic growth at much lower relative humidity than is required for nucleation of pure liquid water droplets from water vapor. Therefore, no nucleation process is involved in real-world cloud droplet formation. In this chapter, we first discuss the concept of hygroscopic growth and then introduce cloud condensation nuclei (CCN) and Köhler theory, that can be used to mathematically describe cloud droplet activation. To understand the Köhler theory, we introduce the Kelvin law and the Raoult’s law as well as the principles of the so-called 𝜅-Köhler theory.
This book studies the emergence of large-scale structure from small structures in the context of random graphs. Typical large graphs with fixed edge density e and triangle density t are described by a 'graphon' that solves a constrained optimization problem. Proofs are provided of the existence of infinitely many open sets ('phases') in the (e,t) plane where the optimal graphon is unique and varies analytically with (e,t). The optimal graphons take a simple form, with symmetries that vary from phase to phase, indicating an emergent self-organization of the corresponding graphs. Besides being of independent interest in the theory of random graphs, extremal combinatorics and the calculus of variations, this provides a rigorous framework for studying ideas from statistical physics that have never been proven in their original setting. The techniques presented in this book can serve as a guide for optimization problems in other fields.
We introduce a new permutation statistic, which we call the k-window statistic, for permutations of $\{1,2,\ldots, n\}$. The aim is to add to the repertoire of potentially useful tools in the design of efficient algorithms. The k-window statistic counts the number of elements that are at a displacement at most k from their natural positions in the ascendingly sorted permutation. We find the exact mean and exact variance of the k-window statistic, revealing phases in the mean and variance in the different regimes of k. We find a weak (or even strong) law of large numbers in the regime where $k=k_n$ is growing but remains ${\mathrm{o}} (n)$. Via a representation of the statistic into dependent heterogeneous weakly correlated indicators, we establish the complete spectrum of distributions as $k_n$ spans its entire range using an appropriate method for each regime.
Chapter 1 explores the most common phases of matter: solid, liquid, and gas. We cover the pressure–temperature phase diagrams that show the boundaries separating these phases. This includes special points such as the critical point and the triple point. Next, we consider the Gibbs free energy and its connection to phase transitions. This leads naturally to the Clausius–Clapeyron equation, which relates the slope of phase boundaries to the entropy and volumes of the coexisting phases. We then turn to pressure–volume phase diagrams, showing explicitly the coexistence that occurs in first-order, discontinuous phase transitions.
An introduction of the four classical models: the voter model, the contact process, stochastic Ising models, and the exclusion process, complemented by some variations on the classical models such as the two-stage contact process or biased and rebellious voter models, as well as some other models such as systems of branching, coalescing, and annihilating random walks and an example of a kinetically constrained model. Some well-known major results are mentioned together with many open problems and topics that are from the mathematical side and still poorly understood, such as the critical exponents associated with continuous phase transition and (in the final section) periodic behavior.
This chapter focuses on research progress related to full quantum effects in dense hydrogen, hydride compounds, and proton transport through 2D materials and bulk materials where hydrogen does not dominate in content. For dense hydrogen, this chapter describes nuclear quantum effects in high-pressure phase diagram, phase transition, and physical property. For the most common hydride compound, water, this chapter introduces nuclear quantum effects in water hydrogen bond property, water phase diagram, and physical and chemical property of confined water and ice. For other hydride compound, this chapter introduces full quantum effects in hydride superconductivity and nonlinear optical property of mineral hydride. These studies reveal that, full quantum effect not only has significant contribution to existing properties, such as hydrogen bond strength and phase diagram boundary probed by isotope substitution, but also causes novel states and properties, such as room temperature, high-pressure superconductivity of hydrides (e.g., sulfur hydride) and liquid forms of metallic and superconducting hydrogen. After these, this chapter introduces theory of proton tunneling rate, which is important from physical to life sciences. Theory of proton transport in perovskite-type oxides is also illustrated as typical example of nuclear quantum effects on hydrogen conduction in bulk materials. Finally, the chapter introduces work demonstrating importance of proton tunneling in DNA mutation.
We consider general continuum percolation models obeying sparseness, translation invariance, and spatial decorrelation. In particular, this includes models constructed on general point sets other than the standard Poisson point process or the Bernoulli-percolated lattice. Moreover, in our setting the existence of an edge may depend not only on the two end vertices but also on a surrounding vertex set and models are included that are not monotone in some of their parameters. We study the critical annulus-crossing intensity $\widehat{\lambda}_\mathrm{c}$, which is smaller than or equal to the classical critical percolation intensity $\lambda_\mathrm{c}$ and derive a condition for $\widehat{\lambda}_\mathrm{c}\gt 0$ by relating the crossing of annuli to the occurrence of long edges. This condition is sharp for models that have a modicum of independence. In a nutshell, our result states that annuli are either not crossed for small intensities or crossed by a single edge. Our proof rests on a multiscale argument that further allows us to directly describe the decay of the annulus-crossing probability with the decay of long-edges probabilities. We apply our result to a number of examples from the literature. Most importantly, we extensively discuss the weight-dependent random connection model in a generalized version, for which we derive sufficient conditions for the presence or absence of long edges that are typically easy to check. These conditions are built on a decay coefficient $\zeta$ that has recently seen some attention due to its importance for various proofs of global graph properties.
We study the activated random walk model on the one-dimensional ring, in the high-density regime. We develop a toppling procedure that gradually builds an environment that can be used to show that activity will be sustained for a long time. This yields a self-contained and relatively short proof of existence of a slow phase for arbitrarily large sleep rates.
Expansive soils, characterized by large montmorillonite (Mnt) contents, exhibit significant swelling-shrinkage behavior, posing engineering challenges in regions with alternating wet and dry seasons, such as southern China. Recent studies have explored the possible use of microbes to control or modify the swelling-shrinkage behavior. This study has evaluated microbial influence on the swelling-shrinkage behaviors of expansive soils. A combination of aqueous phase characterization through inductively coupled plasma-optical emission spectroscopy (ICP-OES) and solid phase analyses including X-ray diffraction (XRD) and Fourier-transform infrared spectroscopy (FTIR) was adopted to elucidate the variations in system parameters. Results showed that Si, Al, K, and Mg concentrations in the supernatant increased with prolonged interaction, with K concentration peaking at 14 days and decreasing to 27.5 mg L−1 at 42 days, indicating K+ uptake by Mnt interlayers. The Si–O bonds in tetrahedral sheets, Al–O bonds in octahedral structures, and –OH bonds in water molecules were disrupted by Paenibacillus mucilaginosus, accelerating the montmorillonite to illite (Mnt-to-Ilt) transformation. An Ilt-Mnt interstratification peak appeared near 9.88°2θ after 14 days, and an Ilt peak emerged at 48.07°2θ after 28 days. The Mnt content decreased by 37.28%, while the Ilt content increased by 104.01% after 42 days, as calculated by the K-value method. Analysis of swelling-shrinkage properties revealed that reduced Mnt content led to a 69.01% decrease in the free swell index and a 24.04% decrease in the swell ratio under load. The linear and volumetric shrinkage ratios decreased by 32.90% and 30.98%, respectively. Microorganisms can promote the weathering and phase transformation of Mnt into non-expansive minerals, thereby reducing the amount of it and thus reducing the swelling-shrinkage potential in expansive soils.
The chapter begins with physics and mathematical description of the nonlinear dynamics seen in biological neurons and their adaptation into neuromorphic hardware. Various abstractions of the Hodgkin–Huxley model of squid neuron have been studied in neuromorphic computing. Filamentary threshold switches that can act as neurons are discussed. The combination of ionic and electronic relaxation pathways offers unique abilities to design low-power artificial neurons. Ferroelectric, insulator–metal transition, 2D materials, and organic semiconductor-based neurons are discussed wherein modulation of long-range transport and/or bound charge displacement are utilized for neuron function. Besides electron transport, light and spin state can also be effectively utilized to create photonic and spintronic neurons respectively. The chapter should provide the reader a comprehensive insight into design of artificial neurons that can generate action potentials, spanning various classes of inorganic and organic semiconductors, and different stimuli for input and readout of signals such as voltage, light, spin current, and ionic currents.
Feldspars are among the most common phases in the Earth’s crust and are characterized by wide variations in chemical composition and crystal structure motifs. In this paper, we synthesized SrZn2P2O8 and studied it by means of scanning electron microscopy, electron microprobe analysis and powder X-ray diffraction at ambient and high-temperature (up to 900°C) conditions. We have structurally characterized for the first time layered triclinic β-modification of SrZn2P2O8 (space group P$\bar 1$, a = 5.0109(8), b = 8.6202(13), c = 9.7527(15) Å, α = 118.088(3), β = 74.622(6), γ = 87.525(6)° and V = 351.29(10) Å3), which is structurally related to hexacelsian. The high-temperature study demonstrated that β-SrZn2P2O8 transformed irreversibly into the framework monoclinic paracelsian-like α-SrZn2P2O8 (space group P21/c, a = 8.3163(2), b = 9.5023(2), c = 9.0248(2) Å, β = 92.285(1)°, V = 712.60(1) Å3) above 600°C, which, in turn, is stable up to 900°C, when it melts. Though the crystal structures of α- and β-modification of SrZn2P2O8 are different (framework and layered, respectively), their thermal expansion is similar: αV ≈ 26 ± 1 × 10–6 °C–1, αmax/αmin ≈ 5. The possible occurrence of the corresponding minerals in nature is discussed.
We study the bilateral preference graphs $\mathit{LK}(n, k)$ of La and Kabkab, obtained as follows. Put independent and uniform [0, 1] weights on the edges of the complete graph $K_n$. Then, each edge (i, j) is included in $\mathit{LK}(n,k)$ if it is bilaterally preferred, in the sense that it is among the k edges of lowest weight incident to vertex i, and among the k edges of lowest weight incident to vertex j. We show that $k = \log(n)$ is the connectivity threshold, solving a conjecture of La and Kabkab, and obtaining finer results about the window. We also investigate the asymptotic behavior of the average degree of vertices in $\mathit{LK}(n, k)$ as $n\rightarrow\infty$.
The leucite group structures are tetrahedrally coordinated silicate framework structures with some of the silicate framework cations partially replaced by divalent or trivalent cations. These structures have general formulae A2BSi5O12 and ACSi2O6, where A is a monovalent alkali metal cation, B is a divalent cation, and C is a trivalent cation. These leucites can have crystal structures in several different space groups, dependent on stoichiometry, synthesis conditions, and temperature. Phase transitions are known for temperature changes. This paper reports a high-temperature X-ray powder diffraction study on RbGaSi2O6, which shows a phase transition from I41/a tetragonal to Iad cubic on heating from room temperature to 733 K. On cooling to room temperature, the crystal structure reverts to I41/a tetragonal.
The foundations of experimental psychology are examined in order to understand how the field of timing came to be focussed on the single fact that people and other animals can, with some accuracy, judge intervals of time. The theories and experiments that have arisen to explain this ability are reviewed. The main theme of the book is then introduced, that the experience of time is quite unlike any other experience by having a phase transition. The phase transition occurs at a time interval of about 2 seconds, and this sets the terms for any discussion of human temporality. Finally, by distinguishing between temporal flow and historical progression, the argument is made that the field of timing has not been studying judgment of time, but rather has been studying judgment of episodic memory.
The role that proximity plays in grouping is examined in both the spatial and temporal domains. It is shown that groups in space behave quite differently than groups in time when they are dilated or expanded. Spatial organization is shown to be scale-free in consequence of the tradeoff between size and distance in spatial vision. Numerous examples from music and the psychological literature are given to show that the apprehension of time is bound to a scale that evaluates to about 2 seconds. Two seconds is shown to act as a watershed, a proximity constraint, for the formation of melody, rhythmic experience, and every other experience that creates bridges in time. The work of Paul Fraisse, a foundational thinker in the field of timing, is highlighted. His thought experiments make appearances throughout the book.
Chlorite plays an essential role in transporting water into the deep Earth. This study investigates the high-pressure behaviour of clinochlore up to ∼20 GPa at room temperature, using synchrotron X-ray diffraction and infrared spectroscopy. We identified a polytypic phase transition (from IIb-2 to IIa-1) at ∼9 GPa and a structural distortion at ∼12 GPa. The polytypic phase transition at ∼9 GPa is characterised by a significant reorganization of interlayer hydrogen bonding, transitioning to states of weakly bonded or non-hydrogen-bonded hydroxyl groups. The phase transition showed reversibility during the experiment. The structural distortion near 12 GPa indicates adjustments in the compression mechanism related to the hydroxyl groups across both the brucite-like and 2:1 sheets. The unit-cell volume of the low-pressure IIb-2 phase was fitted to the second-order Birch-Murnaghan equation of state, and the resulting parameters are V0 = 710.9(3) Å3 and K0 = 83.4(8) GPa. Our results exhibit a marked deviation from prior experimental findings, potentially attributable to the presence of Fe2+ cation incorporation in the natural chlorite investigated in this work. This study emphasises the complexity of the hydroxyl group in response to pressure in layered-structure silicates.
Feldspars are the most common minerals in the Earth’s crust, and commonly contain trace concentrations of gallium and germanium. However, their gallium/germanium synthetic analogues are widely used, both in industrial applications and geological reconstructions. Here KMeGe3O8 (Me = Al, Ga) compounds were synthesized using solid-state reactions and hydrothermal synthesis and studied by microprobe analysis and powder X-ray diffraction (under both ambient and high-temperature conditions). In both (Al and Ga) cases, paracelsian-like phases were the first to form, even though feldspar-like phases are predicted to be thermodynamically stable. Paracelsian-like phases are transformed irreversibly upon heating (930 ± 30 and 960 ± 30°C for KGaGe3O8 and KAlGe3O8, respectively) into feldspar-like modifications. According to the obtained data, the feldspar-like modifications exhibit a higher degree of anisotropy, whereas the volume thermal expansion coefficients are higher for paracelsian-like modifications. The influence of chemical composition and topology on the crystallization process, thermal transformation and thermal expansion of feldspar- and paracelsian-like compounds is discussed.
Groutite, α-Mn3⁺O(OH), is a mineral that belongs to the diaspore group. We used X-ray synchrotron radiation in the pressure range from 0.65(6) GPa to 39.85(8) GPa to collect diffraction data for three single crystals of groutite placed in a diamond anvil cell. Groutite is orthorhombic, space group Pbnm. Analysis of the reciprocal lattice planes and the intensities of the measured reflections revealed that above 30 GPa, a phase transformation begins in the structure. This transition is gradual, with observable changes in the intensity of specific reflections, particularly those that are forbidden in the Cmcm space group. Although we see significant decreases in the intensities of these reflections, many of them still have intensities significantly greater than zero after the beginning of transformation. This is accompanied by a smooth, continuous shrinkage in the unit cell volume, symmetrization of hydrogen positions, and distortion of the MnO6 octahedra. Analysis of the reflection intensities confirms that the observed changes are due to structural transformations and not experimental or sample effects. This means that the starting Pbnm symmetry is preserved although the mineral transforms as a function of pressure close to the Cmcm space-group symmetry. We propose a mechanism for this phase transition in the Pbnm space group.