Searcharxiv⌕ Search

arXiv subjects

Tiago J. Oliveira

Publications and source records attributed to Tiago J. Oliveira.

At least 19 recordsLinked to original sources

Entropy of full covering of the kagome lattice by straight trimers

We consider the number of ways all the sites of a kagome lattice can be covered by non-overlapping linear rigid rods where each rod covers 3 sites. We establish a 2-to-1 correspondence between the configurations of trimers on the kagome lattice to the covering by dimers of a related hexagonal lattice to show that entropy of coverings per trimer $s_{\text{tri,kag}}$ equals the entropy per dimer $ s_{\text{dim,hex}} $, and is given by $ s_{\text{tri,kag}} = s_{\text{dim,hex}} = \frac{1}{2 π} \int_0^{ 2 π/3} \log( 2 + 2 \cos k) dk \approx 0.323065947\ldots$.

cond-mat.stat-mech↗

Dimensional crossover in surface growth on rectangular substrates

In a recent work [Phys. Rev. E 109, L042102 (2024)], interesting dimensional crossovers [from two- to one-dimensional (2D to 1D) scaling] were found in the growth of Kardar-Parisi-Zhang (KPZ) interfaces on rectangular substrates, with lateral sizes $L_y > L_x$. Here, we extend this study to other universality classes for interface growth -- specifically, the Edwards-Wilkinson (EW), the Mullins-Herring (MH), and the Villain-Lai Das Sarma (VLDS) classes. From extensive simulations, we demonstrate that, in all systems with sufficiently large aspect ratio $\mathcal{R}=L_y/L_x$, the roughness $W$ scales with time $t$ in the growth regime as $W \sim t^{β_{\text{2D}}}$ for $t \ll t_c$ and $W \sim t^{β_{\text{1D}}}$ for $t \gg t_c$, where $t_c \sim L_x^{z_{2\text{D}}}$ in most cases. For the VLDS class, this crossover is also observed in the height distribution (HD), which approaches its characteristic probability density function for the 2D case at short times ($t \ll t_c$) and then crosses over to the asymptotic 1D HD. Dimensional crossovers are also found in the steady state regime, both in the roughness scaling as well as in the VLDS HD, which interpolate between the 2D and 1D ones as $\mathcal{R}$ increases. The particular case $L_x = L_y^δ$, with $0 < δ< 1$, is also discussed in detail and reveals interesting features of the investigated systems. For instance, there exist a `special' exponent $δ^* = z_{1\text{D}}/z_{2\text{D}}$ such that the temporal crossover cannot be observed for $δ> δ^*$. Moreover, this leads the saturation roughness to display a nonuniversal scaling: $W_s \sim L_y^Λ$, with $Λ= (1-δ) α_{1\text{D}} + δα_{2\text{D}}$.

cond-mat.stat-mech↗

Universal Coarsening and Giant-Cluster Formation in Growing Interfaces

Clusters formed by fluctuations of two-dimensional (2D) directed interfaces around a threshold level have been extensively studied at equilibrium and in nonequilibrium steady states, but their coarsening dynamics remain poorly understood. Here, we numerically investigate this unexplored coarsening of clusters in 2D growing interfaces believed to belong to the Kardar-Parisi-Zhang universality class. Using a two-point spatial correlator, we demonstrate statistical time invariance of the evolving configurations and identify scaling forms shared across distinct models. We reveal a pronounced asymmetry in the growth of the largest clusters: one cluster emerges as a giant structure whose characteristic length exceeds the correlation length. Population-dependent scaling forms for the number densities of cluster areas are uncovered. These findings highlight new universal aspects of growing interfaces and suggest avenues for experimental verification.

cond-mat.stat-mech↗

Hard rigid rods on Husimi lattices

We study the thermodynamic behavior of hard rigid rods of size $k$ (i.e., $k$-mers) on four- and six-coordinated Husimi lattices (HLs), respectively built with squares (square HL) and triangles (triangular HL). In both lattices, dimers ($k=2$) and trimers ($k=3$) only present a isotropic phase, whereas a isotropic-nematic transition is observed for $k \ge 4$. In the square HL, this transition is continuous and occurs at a critical \textit{monomer} activity which displays a nonmonotonic variation with $k$, while the critical \textit{rod} activity and density are always decreasing functions of $k$. The isotropic-nematic transition is discontinuous in the triangular HL, but the $k$-dependence of the coexistence activities and density is analogous to that found for the square case. No transition from the nematic to a high-density disordered phase is found in these HLs. In general, this scenario is very similar to that already observed for rods on the Bethe lattice, though the critical parameters obtained here are in most cases closer to those reported in the literature for the square and triangular lattices. The entropy per site of fully-packed rods is also investigated in detail in the triangular HL, where its value for dimers differs by only 0.7\% from the exact result for the triangular lattice.

cond-mat.stat-mech↗

Dimensional crossover in Kardar-Parisi-Zhang growth

Two-dimensional (2D) KPZ growth is usually investigated on substrates of lateral sizes $L_x=L_y$, so that $L_x$ and the correlation length ($ξ$) are the only relevant lengths determining the scaling behavior. However, in cylindrical geometry, as well as in flat rectangular substrates $L_x \neq L_y$ and, thus, the surfaces can become correlated in a single direction, when $ξ\sim L_x \ll L_y$. From extensive simulations of several KPZ models, we demonstrate that this yields a dimensional crossover in their dynamics, with the roughness scaling as $W \sim t^{β_{\text{2D}}}$ for $t \ll t_c$ and $W \sim t^{β_{\text{1D}}}$ for $t \gg t_c$, where $t_c \sim L_x^{1/z_{2\text{D}}}$. The height distributions (HDs) also cross over from the 2D flat [cylindrical] HD to the asymptotic Tracy-Widom GOE [GUE] distribution. Moreover, 2D-to-1D crossovers are found also in the asymptotic growth velocity and in the steady state regime of flat systems, where a family of universal HDs exists, interpolating between the 2D and 1D ones as $L_y/L_x$ increases. Importantly, the crossover scalings are fully determined and indicate a possible way to solve 2D KPZ models.

cond-mat.stat-mech↗

On the universality class of the special adsorption point of two-dimensional lattice polymers

In recent work [PRE 100, 022121 (2019)] evidence was found that the surface adsorption transition of interacting self-avoiding trails (ISATs) placed on the square lattice displays a non-universal behavior at the special adsorption point (SAP) where the collapsing polymers adsorb. In fact, different surface exponents $ϕ^{(s)}$ and $1/δ^{(s)}$ were found at the SAP depending on whether the surface orientation is horizontal (HS) or diagonal (DS). Here, we revisit these systems and study other ones, through extensive Monte Carlo simulations, considering much longer trails than previous works. Importantly, we demonstrate that the different exponents observed in the reference above are due to the presence of a previously unseen surface-attached-globule (SAG) phase in the DS system, which changes the multicritical nature of the SAP and is absent in the HS case. By considering a modified horizontal surface (mHS) where the trails are forbidden of having two consecutive steps along it, resembling the DS situation, a stable SAG phase is found in the phase diagram, and both DS and mHS systems present similar $1/δ^{(s)}$ exponents at the SAP, being $1/δ^{(s)} \approx 0.44$, whilst $1/δ^{(s)} \approx 0.34$ in the HS case. Intriguingly, while $ϕ^{(s)} \approx 1/δ^{(s)}$ is found for the DS and HS scenarios, as expected, in the mHS case $ϕ^{(s)}$ is about $10$\% smaller than $1/δ^{(s)}$. These results strongly indicate that at least two universality classes exist for the SAPs of adsorbing ISATs on the square lattice.

cond-mat.soft↗

One-point height fluctuations and two-point correlators of $(2+1)$ cylindrical KPZ systems

While the 1-point height distributions (HDs) and 2-point covariances of $(2+1)$ KPZ systems have been investigated in several recent works for flat and spherical geometries, for the cylindrical one the HD was analyzed for few models and nothing is known about the spatial and temporal covariances. Here, we report results for these quantities, obtained from extensive numerical simulations of discrete KPZ models, for three different setups yielding cylindrical growth. Beyond demonstrating the universality of the HD and covariances, our results reveal other interesting features of this geometry. For example, the spatial covariances measured along the longitudinal and azimuthal directions are different, with the former being quite similar to the curve for flat $(2+1)$ KPZ systems, while the latter resembles the Airy$_2$ covariance of circular $(1+1)$ KPZ interfaces. We also argue (and present numerical evidence) that, in general, the rescaled temporal covariance $\mathcal{A}(t/t_0)$ decays asymptotically as $\mathcal{A}(x) \sim x^{-\barλ}$ with an exponent $\barλ = β+ d^*/z$, where $d^*$ is the number of interface sides kept fixed during the growth (being $d^* = 1$ for the systems analyzed here). Overall, these results complete the picture of the main statistics for the $(2+1)$ KPZ class.

cond-mat.stat-mech↗

Kardar-Parisi-Zhang universality class in ($d+1$)-dimensions

The determination of the exact exponents of the KPZ class in any substrate dimension $d$ is one of the most important open issues in Statistical Physics. Based on the behavior of the dimensional variation of some exact exponent differences for other growth equations, I find here that the KPZ growth exponents (related to the temporal scaling of the fluctuations) are given by $β_d = \frac{7}{8d+13}$. These exponents present an excellent agreement with the most accurate estimates for them in the literature. Moreover, they are confirmed here through extensive Monte Carlo simulations of discrete growth models and real space renormalization group (RG) calculations for directed polymers in random media (DPRM), up to $d=15$. The left-tail exponents of the probability density functions for the DPRM energy provide another striking verification of the analytical result above.

cond-mat.stat-mech↗

Kardar-Parisi-Zhang growth on square domains that enlarge nonlinearly in time

We study discrete KPZ growth models deposited on square lattice substrates, whose (average) lateral size enlarges as $L= L_0 + ωt^γ$. Our numerical simulations reveal that the competition between the substrate expansion and the increase of the correlation length parallel to the substrate, $ξ\simeq c t^{1/z}$, gives rise to a number of interesting results. For instance, when $γ< 1/z$ the interface becomes fully correlated, but its squared roughness, $W_2$, keeps increasing as $W_2 \sim t^{2αγ}$, as previously observed for 1D systems. A careful analysis of this scaling, accounting for an intrinsic width on it, allows us to estimate the roughness exponent of the 2D KPZ class as $α= 0.387(1)$, which is very accurate and robust, once it was obtained averaging the exponents for different models and growth conditions (i.e., for various $γ$'s and $ω$'s). In this correlated regime, the height distributions (HDs) and spatial covariances are consistent with those expected for the steady-state regime of the 2D KPZ class for flat geometry. For $γ\approx 1/z$, we find a family of distributions and covariances continuously interpolating between those for the steady-state and the growth regime of radial KPZ interfaces, as the ratio $ω/c$ augments. When $γ>1/z$ the system stays forever in the growth regime and the HDs always converge to the same asymptotic distribution, which is the one for the radial case. The spatial covariances, on the other hand, are $(γ,ω)$-dependent, showing a trend towards the covariance of a random deposition in enlarging substrates as the expansion rate increases. These results considerably generalize our understanding of the height fluctuations in 2D KPZ systems, revealing a scenario very similar to the one previously found in the 1D case.

cond-mat.stat-mech↗

Height distributions in interface growth: The role of the averaging process

To quantitatively characterize height distributions (HDs), one uses adimensional ratios of their first central moments ($m_n$) or cumulants ($κ_n$), especially the skewness $S$ and kurtosis $K$, whose accurate estimate demands an averaging over all $L^d$ points of the height profile at a given time, in translation-invariant interfaces, and over $N$ independent samples. One way of doing this is by calculating $m_n(t)$ [or $κ_n(t)$] for each sample and then carrying out an average of them for the $N$ interfaces, with $S$ and $K$ being calculated only at the end. Another approach consists in directly calculating the ratios for each interface and, then, averaging the $N$ values. It turns out, however, that $S$ and $K$ for the growth regime HDs display strong finite-size and -time effects when estimated from these "interface statistics", as already observed in some previous works and clearly shown here, through extensive simulations of several discrete growth models belonging to the EW and KPZ classes on 1D and 2D substrates of sizes $L=const.$ and $L \sim t$. Importantly, I demonstrate that with "1-point statistics'', i.e., by calculating $m_n(t)$ [or $κ_n(t)$] once for all $N L^d$ heights together, these corrections become very weak. However, I find that this "1-point'' approach fails in uncovering the universality of the HDs in the steady state regime (SSR) of systems whose average height, $\bar{h}$, is a fluctuating variable. In fact, as demonstrated here, in this regime the 1-pt height evolves as $h(t) = \bar{h}(t) + s_λ A^{1/2} L^α ζ+ \cdots$ -- where $P(ζ)$ is the underlying SSR HD -- and the fluctuations in $\bar{h}$ yield $S_{1pt} \sim t^{-1/2}$ and $K_{1pt} \sim t^{-1}$. Nonetheless, by analyzing $P(h-\bar{h})$, the cumulants of $P(ζ)$ can be accurately determined.

cond-mat.stat-mech↗

Semianalytical solutions of Ising-like and Potts-like magnetic polymers on the Bethe lattice

We study magnetic polymers, defined as self-avoiding walks where each monomer $i$ carries a "spin'' $s_i$ and interacts with its first neighbor monomers, let us say $j$, via a coupling constant $J(s_i,s_j)$. Ising-like [$s_i = \pm 1$, with $J(s_i,s_j) = \varepsilon s_i s_j$] and Potts-like [$s_i = 1,\ldots,q$, with $J(s_i,s_j)=\varepsilon_{s_i} δ(s_i,s_j)$] models are investigated. Some particular cases of these systems have recently been studied in the continuum and on regular lattices, and are related to interesting applications. Here, we solve these models on Bethe lattices of ramification $σ$, focusing on the ferromagnetic case in zero external magnetic field. In most cases, the phase diagrams present a non-polymerized (NP) and two polymerized phases: a paramagnetic (PP) and a ferromagnetic (FP) one. However, quite different thermodynamic properties are found depending on $q$ in the Potts-like polymers and on whether one uses the Ising or Potts coupling in the two-state systems. Importantly, these results indicate that when $q\le 6$ the spin ordering transition is preceded by the polymer collapse transition, whereas for $q\ge 7$ and in the Ising case these transitions happen together at critical-end-points. Some interesting non-standard Potts models are also studied, such as the lattice version of the model for epigenetic marks in the chromatin introduced in [PRX {\bf 6}, 041047 (2016)]. In addition, the solution of the dilute Ising and dilute Potts models on the Bethe lattice are also presented here, once they are important to understand the PP-FP transitions.

cond-mat.stat-mech↗

Entropy of fully-packed rigid rods on generalized Husimi trees: a route to the square lattice limit

Although hard rigid rods ($k$-mers) defined on the square lattice have been widely studied in the literature, their entropy per site, $s(k)$, in the full-packing limit is only known exactly for dimers ($k=2$) and numerically for trimers ($k=3$). Here, we investigate this entropy for rods with $k \le 7$, by defining and solving them on Husimi lattices built with diagonal and regular square lattice clusters of effective lateral size $L$, where $L$ defines the level of approximation to the square lattice. Due to an $L$-parity effect, by increasing $L$ we obtain two systematic sequences of values for the entropies $s_L(k)$ for each type of cluster, whose extrapolations to $L \rightarrow \infty$ provide estimates of these entropies for the square lattice. For dimers, our estimates for $s(2)$ differ from the exact result by only $0.03\%$, while that for $s(3)$ differs from best available estimates by $3\%$. In this paper, we also obtain a new estimate for $s(4)$. For larger $k$, we find that the extrapolated results from the Husimi tree calculations do not lie between the lower and upper bounds established in the literature for $s(k)$. In fact, we observe that, to obtain reliable estimates for these entropies, we should deal with levels $L$ that increase with $k$. However, it is very challenging computationally to advance to solve the problem for large values of $L$ and for large rods. In addition, the exact calculations on the generalized Husimi trees provide strong evidence for the fully packed phase to be disordered for $k\geq 4$, in contrast to the results for the Bethe lattice wherein it is nematic, thus providing evidence for a high density nematic-disordered transition in the system of $k$-mers with vacancies.

cond-mat.stat-mech↗

Husimi lattice solutions and the coherent-anomaly-method analysis for hard-square lattice gases

Although lattice gases composed by $k$NN particles, forbidding up to their $k$th nearest neighbors of being occupied, have been widely investigated in literature, the location and the universality class of the fluid-columnar transition in the 2NN model on the square lattice is still a topic of debate. Here, we present grand-canonical solutions of this model on Husimi lattices built with diagonal square lattices, with $2L(L+1)$ sites, for $L \leqslant 7$. The systematic sequence of mean-field solutions confirms the existence of a continuous transition in this system and extrapolations of the critical chemical potential $μ_{2,c}(L)$ and particle density $ρ_{2,c}(L)$ to $L \rightarrow \infty$ yield estimates of these quantities in close agreement with previous results for the 2NN model on the square lattice. To confirm the reliability of this approach we employ it also for the 1NN model, where very accurate estimates for the critical parameters $μ_{1,c}$ and $ρ_{1,c}$ -- for the fluid-solid transition in this model on the square lattice -- are found from extrapolations of data for $L \leqslant 6$. The non-classical critical exponents for these transitions are investigated through the coherent anomaly method (CAM), which in the 1NN case yields $β$ and $ν$ differing by at most 6\% from the expected Ising exponents. For the 2NN model, the CAM analysis is somewhat inconclusive, because the exponents sensibly depend on the value of $μ_{2,c}$ used to calculate them. Notwithstanding, our results suggest that $β$ and $ν$ are considerably larger than the Ashkin-Teller exponents reported in numerical studies of the 2NN system.

cond-mat.stat-mech↗

Surface growth on treelike lattices and the upper critical dimension of the KPZ class

Aiming to investigate the upper critical dimension, $d_u$, of the KPZ class, in [EPL 103 (2013) 10005] some growth models were numerically analyzed using Cayley trees (CTs) as substrates, as a way to access their behavior in the infinite-dimensional limit, and some unexpected results were reported: logarithmic roughness scaling, differing for EW and KPZ models (indicating that even at $d=\infty$ the KPZ nonlinearity is still relevant); beyond asymptotically rough EW surfaces above the upper critical dimension of the EW class. Motivated by these strange findings, I revisit these growth models here to show that such results are simple consequences of boundary effects, inherent to systems defined on CTs. In fact, I demonstrate that the anomalous boundary of the CT leads the growing surfaces to develop curved shapes, which explains the strange behaviors previously found for these systems, once the global "roughness" were analyzed for non-flat surfaces in the study above. Importantly, by measuring the height fluctuations at the central site of the CT, which can be seen as an approximation for the Bethe lattice, smooth surfaces are found for both EW and KPZ classes, consistently with the behavior expected for growing systems in dimensions $d \geqslant d_u$. Interesting features of the 1-pt height fluctuations, such as the possibility of non-saturation in the steady state regime, are also discussed for substrates in general.

cond-mat.stat-mech↗

Fluid-fluid demixing and density anomaly in a ternary mixture of hard spheres

We report the grand-canonical solution of a ternary mixture of discrete hard spheres defined on a Husimi lattice built with cubes, which provides a mean-field approximation for this system on the cubic lattice. The mixture is composed by point-like particles (0NN) and particles which exclude up to their first (1NN) and second neighbors (2NN), with activities $z_0$, $z_1$ and $z_2$, respectively. Our solution reveals a very rich thermodynamic behavior, with two solid phases associated with the ordering of 1NN ($S1$) or 2NN particles ($S2$), and two fluid phases, being one regular ($RF$) and the other characterized by a dominance of 0NN particles ($F0$ phase). However, in most part of the phase diagram these fluid ($F$) phases are indistinguishable. Discontinuous transitions are observed between all the four phases, yielding several coexistence surfaces in the system, among which a fluid-fluid and a solid-solid demixing surface. The former one is limited by a line of critical points and a line of triple points (where the phases $RF$-$F0$-$S2$ coexist), both meeting at a special point, after which the fluid-fluid coexistence becomes metastable. Another line of triple points is found, connecting the $F$-$S1$, $F$-$S2$ and $S1$-$S2$ coexistence surfaces. A critical $F$-$S1$ surface is also observed meeting the $F$-$S1$ coexistence one at a line of tricritical points. Furthermore, a thermodynamic anomaly characterized by minima in isobaric curves of the total density of particles is found, yielding three surfaces of minimal density in the activity space, depending on which activity is kept fixed during its calculation.

cond-mat.soft↗

Adsorption of 2d polymers with two- and three-body self-interactions

Using extensive Monte Carlo simulations, we investigate the surface adsorption of self-avoiding trails on the triangular lattice with two- and three-body on-site monomer-monomer interactions. In the parameter space of two-body, three-body, and surface interaction strengths, the phase diagram displays four phases: swollen (coil), globule, crystal, and adsorbed. For small values of the surface interaction, we confirm the presence of swollen, globule, and crystal bulk phases. For sufficiently large values of the surface interaction, the system is in an adsorbed state, and the adsorption transition can be continuous or discontinuous, depending on the bulk phase. As such, the phase diagram contains a rich phase structure with transition surfaces that meet in multicritical lines joining in a single special multicritical point. The adsorbed phase displays two distinct regions with different characteristics, dominated by either single or double layer adsorbed ground states. Interestingly, we find that there is no finite-temperature phase transition between these two regions though rather a smooth crossover.

cond-mat.stat-mech↗

Thermodynamic behavior of binary mixtures of hard spheres: Semianalytical solutions on a Husimi lattice built with cubes

We study binary mixtures of hard particles, which exclude up to their $k$th nearest neighbors ($k$NN) on the simple cubic lattice and have activities $z_k$. In the first model analyzed, point particles (0NN) are mixed with 1NN ones. The grand-canonical solution of this model on a Husimi lattice built with cubes unveils a phase diagram with a fluid and a solid phase separated by a continuous and a discontinuous transition line which meet at a tricritical point. A density anomaly, characterized by minima in isobaric curves of the total density of particles against $z_0$ (or $z_1$), is also observed in this system. Overall, this scenario is identical to the one previously found for this model when defined on the square lattice. The second model investigated consists of the mixture of 1NN particles with 2NN ones. In this case, a very rich phase behavior is found in its Husimi lattice solution, with two solid phases - one associated with the ordering of 1NN particles ($S1$) and the other with the ordering of 2NN ones ($S2$) -, beyond the fluid ($F$) phase. While the transitions between $F$-$S2$ and $S1$-$S2$ phases are always discontinuous, the $F$-$S1$ transition is continuous (discontinuous) for small (large) $z_2$. The critical and coexistence $F$-$S1$ lines meet at a tricritical point. Moreover, the coexistence $F$-$S1$, $F$-$S2$ and $S1$-$S2$ lines meet at a triple point. Density anomalies are absent in this case.

cond-mat.soft↗

Three stable phases and thermodynamic anomaly in a binary mixture of hard particles

While the realistically modeling of the thermodynamic behavior of fluids usually demands elaborated atomistic models, much have been learned from simplified ones. Here, we investigate a model where point-like particles (with activity $z_0$) are mixed with molecules that exclude their first and second neighbors (i.e., cubes of lateral size $λ=\sqrt{3}a$, with activity $z_2$), both placed on the sites of a simple cubic lattice with parameter $a$. Only hard-core interactions exist among the particles, so that the model is athermal. Despite its simplicity, the grand-canonical solution of this model on a Husimi lattice built with cubes revels a fluid-fluid demixing, yielding a phase diagram with two fluid phases (one of them dominated by small particles - $F0$) and a solid-like phase coexisting at a triple-point. Moreover, the fluid-fluid coexistence line ends at a critical point. An anomaly in the total density ($ρ_T$) of particles is also found, which is hallmarked by minima in the isobaric curves of $ρ_T$ versus $z_0$ (or $z_2$). Interestingly, the line of minimum density cross the phase diagram starting inside the region where both fluid phases are stable, passing through the $F0$ one and ending deep inside its metastable region, in a point where the spinodals of both fluid phases cross each other.

cond-mat.soft↗