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Oleg Alekseev

Publications and source records attributed to Oleg Alekseev.

16 recordsLinked to original sources

Local Rank-One Logarithmic Instability for the Mixed Hessian of the Dispersionless Toda $τ$-Function

We study a weighted renormalization of the mixed Hessian of the dispersionless Toda $τ$-function associated with polynomial conformal maps. The starting point is an explicit logarithmic-kernel representation, which yields a decomposition of the Hessian into symmetry blocks and reduces the spectral analysis to the inverse-map generating function $U(x;ζ)$ and the geometry of its dominant singularities. Near a transversal subcritical approach to a simple analytic critical point, we identify a rank-one logarithmic spectral instability: in each renormalized symmetry block, exactly one variational eigenvalue diverges logarithmically, whereas the remaining variational eigenvalues stay bounded. The proof isolates the analytic mechanism behind this transition in the emergence of a dominant $s$-orbit of simple square-root branch points of the Taylor branch of the inverse map. We then apply the same framework to reduced Laplacian-growth trajectories and show that the same spectral transition occurs there under the same local continuation hypotheses. If, in addition, the reduced map remains univalent at the spectral crossing, then this transition occurs before geometric breakdown. The result is local and conditional: it identifies the mechanism of the first instability and formulates an abstract criterion for extensions beyond the polynomial class.

math-ph

Spectral Structure of the Mixed Hessian of the Dispersionless Toda $τ$-Function

We study the mixed Hessian of the dispersionless Toda $τ$-function for the one-harmonic $s$-fold symmetric conformal map $f(w)=rw+aw^{1-s}$. This Hessian is the susceptibility matrix generated by the inverse conformal map. Our spectral statements are formulated for its weighted symmetry-block realizations on a fixed Hilbert space. In that realization, the first spectral transition occurs at the analytic threshold $ζ_c=(s-1)^{s-1}/s^s$, where the dominant square-root singularity of the inverse map reaches the normalization circle, rather than at the geometric threshold $ζ_{\mathrm{univ}}=1/(s-1)$, where univalence fails. After symmetry decomposition and weighted realization, each block develops exactly one logarithmically diverging eigenvalue as $ζ\uparrowζ_c$, while the remaining spectrum stays bounded and converges to a compact limit. The instability is therefore rank one in every symmetry sector of the weighted block theory. We then continue the scalar Gram generating functions beyond $ζ_c$. They are generalized hypergeometric functions on the slit plane $\mathbb{C}\setminus[ζ_c^2,\infty)$, their branch-point expansion contains the logarithmic term responsible for the divergence, and in the range $1\le p\le s$ they admit Cauchy--Stieltjes and Jacobi-matrix realizations. In particular, the continued scalar quantities remain regular at $ζ_{\mathrm{univ}}$, so the analytic spectral transition strictly precedes the geometric breakdown of univalence.

math-ph

Variational Pattern Selection

We address pattern selection problems in nonlinear interface dynamics by maximizing the entropy of the most probable (classical) scenario associated with the processes. This variational principle we applied to well-known selection problems in a Hele-Shaw cell: stationary Saffman-Taylor finger in a channel and self-similar finger in a wedge. The obtained results excellently agree with experiments. We also address the universal fjord opening angle. This principle complements a non-variational selection developed earlier. Surface tension is not needed for selection in both approaches, contrary to the common belief.

nlin.PS

Universality of stochastic Laplacian growth

We consider a stochastic Laplacian growth problem in the framework of normal random matrices. In the large $N$ limit the support of eigenvalues of random matrices is a planar domain with a sharp boundary which evolves under a change in the size of matrices. This evolution can be interpreted as a stochastic growth process. We show that the most probable growth scenario is similar to deterministic Laplacian growth. The other scenarios involve Laplacian growth in the presence of fluctuations. We use the random matrix approach to determine a probability distribution function of fluctuations. The partition function of fluctuations is shown to be universal. It does not depend on the shape of the initial domain and depends on the strength of fluctuations and the geometry of the problem only.

math-ph

Multi-point passage probabilities and Green's functions for SLE${}_{8/3}$

We consider a loop representation of the $O(n)$ model at the critical point. When $n=0$ the model represents ensembles of self-avoiding loops (i.e., it corresponds to SLE with $κ=8/3$), and can be described by the logarithmic conformal field theory (LCFT) with central charge $c=0$. We focus on the correlation functions in the upper-half plane containing the twist operators in the bulk, and a pair of the boundary one-leg operators. By using a Coulomb gas representation for the correlation functions, we obtain explicit results for probabilities of the SLE${}_{8/3}$ trace to wind in various ways about $N\geq 1$ marked points. When the points collapse pairwise the probabilities reduce to multi-point Green's functions. We propose an explicit representation for the Green's functions in terms of the correlation functions of the bulk 1/3-weight operators, and a pair of the boundary one-leg operators.

math-ph

Martingales of stochastic Laplacian growth

A family of exponential martingales of a stochastic Laplacian growth problem is proposed. Stochastic Laplacian growth describes a regularized interface dynamics in a two-fluid system, where the viscous fluid is incompressible at a large scale, while compressible at a small scale in the vicinity of the interface. Hence, random fluctuations of pressure near the boundary are inevitable. By using Loewner-Kufarev equation, we study interface dynamics generated by nonlocal random Loewner measure, which produces the patterns with viscous fingers. We use a Schottky double construction to introduce a one-parametric family of functions of random processes on the double closely connected to the correlation functions of primary operators of the boundary conformal field theory in the Coulomb gas framework. For a specific value of the parameter, these functions are martingales with respect to stochastic Loewner flow on the Schottky double. A connection between the proposed algebraic construction and the physical problem of stochastic interface dynamics relies on the Hadamard's variational formula. Namely, the variation of pressure in stochastic Laplacian growth near the interface is given by the covariance of martingales on the double.

math-ph

Quantized Laplacian growth, III: On conformal field theories of Laplacian growth

A one-parametric stochastic dynamics of the interface in the quantized Laplacian growth with zero surface tension is introduced. The quantization procedure regularizes the growth by preventing the formation of cusps at the interface, and makes the interface dynamics chaotic. In a long time asymptotic, by coupling a conformal field theory to the stochastic growth process we introduce a set of observables (the martingales), whose expectation values are constant in time. The martingales are connected to degenerate representations of the Virasoro algebra, and can be written in terms of conformal correlation functions. A direct link between Laplacian growth and the conformal Liouville field theory with the central charge $c\geq25$ is proposed.

cond-mat.stat-mech

Quantized Laplacian growth, I: Statistical theory of Laplacian growth

We regularize the Laplacian growth problem with zero surface tension by introducing a short-distance cutoff $\hbar$, so that the change of the area of domains is quantized and equals an integer multiple of the area quanta $\hbar$. The domain can be then considered as an aggregate of tiny particles (area quanta) obeying the Pauli exclusion principle. The statistical theory of Laplacian growth is introduced by using Laughlin's description of the integer quantum Hall effect. The semiclassical evolution of the aggregate is similar to classical deterministic Laplacian growth. However, the quantization procedure generates inevitable fluctuations at the edge of the droplet. The statistical properties of the edge fluctuations are universal and common to that of quantum chaotic systems, which are generally described by Dyson's circular ensembles on symmetric unitary matrices.

cond-mat.stat-mech

Quantized Laplacian growth, II: 1D hydrodynamics of the Loewner density

A systematic analytic treatment of fluctuations in Laplacian growth is given. The growth process is regularized by a short-distance cutoff $\hbar$ preventing the cusps production in a finite time. This regularization mechanism generates tiny inevitable fluctuations on a microscale, so that the interface dynamics becomes chaotic. The time evolution of fluctuations can be described by the universal Dyson Brownian motion, which reduces to the complex viscous Burgers equation in the hydrodynamic approximation. Because of the intrinsic instability of the interface dynamics, tiny fluctuations of the interface on a microscale generate universal patterns with well developed fjords and fingers in a long time asymptotic.

cond-mat.stat-mech

Statistical mechanics of stochastic growth phenomena

We develop statistical mechanics for stochastic growth processes as applied to Laplacian growth by using its remarkable connection with a random matrix theory. The Laplacian growth equation is obtained from the variation principle and describes adiabatic (quasi-static) thermodynamic processes in the two-dimensional Dyson gas. By using Einstein's theory of thermodynamic fluctuations we consider transitional probabilities between thermodynamic states, which are in a one-to-one correspondence with planar domains. Transitions between these domains are described by the stochastic Laplacian growth equation, while the transitional probabilities coincide with the free-particle propagator on the infinite dimensional complex manifold with the Kähler metric.

cond-mat.stat-mech

Theory of stochastic Laplacian growth

We generalize the diffusion-limited aggregation by issuing many randomly-walking particles, which stick to a cluster at the discrete time unit providing its growth. Using simple combinatorial arguments we determine probabilities of different growth scenarios and prove that the most probable evolution is governed by the deterministic Laplacian growth equation. A potential-theoretical analysis of the growth probabilities reveals connections with the tau-function of the integrable dispersionless limit of the two-dimensional Toda hierarchy, normal matrix ensembles, and the two-dimensional Dyson gas confined in a non-uniform magnetic field. We introduce the time-dependent Hamiltonian, which generates transitions between different classes of equivalence of closed curves, and prove the Hamiltonian structure of the interface dynamics. Finally, we propose a relation between probabilities of growth scenarios and the semi-classical limit of certain correlation functions of "light" exponential operators in the Liouville conformal field theory on a pseudosphere.

cond-mat.stat-mech

Stochastic Laplacian growth

A point source on a plane constantly emits particles which rapidly diffuse and then stick to a growing cluster. The growth probability of a cluster is presented as a sum over all possible scenarios leading to the same final shape. The classical point for the action, defined as a minus logarithm of the growth probability, describes the most probable scenario and reproduces the Laplacian growth equation, which embraces numerous fundamental free boundary dynamics in non-equilibrium physics. For non-classical scenarios we introduce virtual point sources, in which presence the action becomes the Kullback-Leibler entropy. Strikingly, this entropy is shown to be the sum of electrostatic energies of layers grown per elementary time unit. Hence the growth probability of the presented non-equilibrium process obeys the Gibbs-Boltzmann statistics, which, as a rule, is not applied out from equilibrium. Each layer's probability is expressed as a product of simple factors in an auxiliary complex plane after a properly chosen conformal map. The action at this plane is a sum of Robin functions, which solve the Liouville equation. At the end we establish connections of our theory with the tau-function of the integrable Toda hierarchy and with the Liouville theory for non-critical quantum strings.

cond-mat.stat-mech

Wilson Loop Invariants from $W_N$ Conformal Blocks

Knot and link polynomials are topological invariants calculated from the expectation value of loop operators in topological field theories. In 3D Chern-Simons theory, these invariants can be found from crossing and braiding matrices of four-point conformal blocks of the boundary 2D CFT. We calculate crossing and braiding matrices for $W_N$ conformal blocks with one component in the fundamental representation and another in a rectangular representation of $SU(N)$, which can be used to obtain HOMFLY knot and link invariants for these cases. We also discuss how our approach can be generalized to invariants in higher-representations of $W_N$ algebra.

hep-th

Form factors of descendant operators in the Bullough-Dodd model

We propose a free field representation for the form factors of descendant operators in the Bullough-Dodd model. This construction is a particular modification of Lukyanov's technique for solving the form factors axioms. We prove that the number of proposed solutions in each level subspace of the chiral sectors coincide with the number of the corresponding descendant operators in the Lagrangian formalism. We check that these form factors possess the cluster factorization property. Besides, we propose an alternative free field representation which allows us to study analytic properties of the form factors effectively. In particular, we prove that the form factors satisfy non trivial identities known as the "reflection relations". We show the existence of the reflection invariant basis in the level subspaces for a generic values of the parameters.

hep-th

Form factors in the Bullough-Dodd related models: The Ising model in a magnetic field

We consider particular modification of the free-field representation of the form factors in the Bullough-Dodd model. The two-particles minimal form factors are excluded from the construction. As a consequence, we obtain convenient representation for the multi-particle form factors, establish recurrence relations between them and study their properties. The proposed construction is used to obtain the free-field representation of the lightest particles form factors in the $Φ_{1,2}$ perturbed minimal models. As a significant example we consider the Ising model in a magnetic field. We check that the results obtained in the framework of the proposed free-field representation are in agreement with the corresponding results obtained by solving the bootstrap equations.

hep-th

Form factors of descendant operators: $A^{(1)}_{L-1}$ affine Toda theory

In the framework of the free field representation we obtain exact form factors of local operators in the two-dimensional affine Toda theories of the $A^{(1)}_{L-1}$ series. The construction generalizes Lukyanov's well-known construction to the case of descendant operators. Besides, we propose a free field representation with a countable number of generators for the `stripped' form factors, which generalizes the recent proposal for the sine/sinh-Gordon model. As a check of the construction we compare numbers of the operators defined by these form factors in level subspaces of the chiral sectors with the corresponding numbers in the Lagrangian formalism. We argue that the construction provides a correct counting for operators with both chiralities. At last we study the properties of the operators with respect to the Weyl group. We show that for generic values of parameters there exist Weyl invariant analytic families of the bases in the level subspaces.

hep-th