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A locally-built, LLM-digested index of recent arXiv papers in quant finance, geometry/topology, and statistical ML — keyword search served straight from SQLite on this machine.

168,694 papers · 148 categories

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11223344 · May 202619922001200920172026
48 results for third-order evolution

New equations describe surfaces with constant curvature.

problem Characterizing and classifying third-order evolution systems for pseudospherical and spherical surfaces.
method Integrability conditions of g\mathfrak{g}-valued linear problems, with g=sl(2,R)\mathfrak{g}=\mathfrak{sl}(2,\R) or g=su(2)\mathfrak{g}=\mathfrak{su}(2).
result Characterization and classification of systems, including new families of coupled KdV and mKdV-type equations.

For a scalar evolution equation ut=K(t,x,u,ux,,un),n2u_t=K(t,x,u,u_x,\ldots, u_n), n\geq 2 the cohomology spaces H1,s(R)H^{1,s}({\mathcal R}^\infty) vanishes for s3s\geq 3 while the space H1,2(R)H^{1,2}({\mathcal R}^\infty) is isomorphic to the space of variational operators. The cohomology space H1,2(R)H^{1,2}({\mathcal R}^\infty) is also shown to be …

2019-02-08abs ↗pdf ↗

We compute the characteristic Cartan connection associated with a system of third order ODEs. Our connection is different from Tanaka normal one, but still is uniquely associated with the system of third order ODEs. This allows us to find all fundamental invariants of a system of third order ODEs and, in particular, de…

2011-04-05abs ↗pdf ↗

This paper is devoted to a third order study of the end-point map in sub-Riemannian geometry. We first prove third order open mapping results for maps from a Banach space into a finite dimensional manifold. In a second step, we compute the third order term in the Taylor expansion of the end-point map and we specialize …

2019-07-25abs ↗pdf ↗

Minimal surfaces in third-order ODEs identified for linear second-order ODEs.

problem Characterizing minimal surfaces in third-order ODEs.
method Analyzing submanifolds of third-order ODEs as Riemannian manifolds.
result Linear second-order ODEs with y=±y+β(x)y''=\pm y+β(x) are the only minimal surfaces and totally geodesic.

New variational principles found for conformal geodesics.

problem Challenges in Lagrangian formulation for conformal geodesics.
method Enlarging the class of variations leads to a variational formulation with a third-order conformally invariant Lagrangian.
result Some integral curves of the fourth-order ODE system are spirals.

Third-order symmetric Lorentzian manifolds, i.e. Lorentzian manifold with zero third derivative of the curvature tensor, are classified. These manifolds are exhausted by a special type of pp-waves, they generalize Cahen-Wallach spaces and second-order symmetric Lorentzian spaces.

2014-07-14abs ↗pdf ↗

Study third order Einstein deformations for Kähler-Einstein metrics on compact manifolds.

problem Existence of non-trivial Einstein deformations of Kähler metrics.
method Explicitly determined the obstruction to third order Einstein deformation and formulated it in terms of polynomial identities.
result Third order integrability for the Einstein equation is equivalent to Maurer-Cartan type equations and polynomial identities.

We introduce an alternative approach to the third order helicity of a volume preserving vector field BB, which leads us to a lower bound for the L2L^2-energy of BB. The proposed approach exploits correspondence between the Milnor μˉ123\barμ_{123}-invariant for 3-component links and the homotopy invariants of maps to con…

2008-08-11abs ↗pdf ↗

We discuss contact invariant structures on the space of solutions of a third-order ordinary differential equation. Associated to any third-order differential equation modulo contact transformations, Chern introduced a degenerate conformal Lorentzian metric on the space of 2-jets of functions of one variable. When the W…

2010-01-01abs ↗pdf ↗

Based on the theory of Poisson vertex algebras we calculate skew-symmetry conditions and Jacobi identities for a class of third-order nonlocal operators of differential-geometric type. Hamiltonian operators within this class are defined by a Monge metric and a skew-symmetric two-form satisfying a number of differential…

2018-05-02abs ↗pdf ↗

For CR structures in dimension three, the CR pluriharmonic functions are characterized by the vanishing of a third order operator. This third order operator, after composition with the divergence operator, gives the fourth order analogue of the Paneitz operator. In this short note, we give criteria under which the kern…

2015-02-06abs ↗pdf ↗

This article is dedicated to solve the equivalence problem for two third order differential operators on the line under general fiber--preserving transformation using the Cartan method of equivalence. We will do three versions of the equivalence problems: first via the direct equivalence problem, second equivalence pro…

2011-01-17abs ↗pdf ↗

We address the problem of local geometry of third order ODEs modulo contact, point and fibre-preserving transformations of variables. Several new and already known geometries are described in a uniform manner by the Cartan method of equivalence. This includes conformal, Weyl and metric geometries in three and six dimen…

2009-02-24abs ↗pdf ↗

Study shows the second fundamental form of pseudospherical surfaces is universal and not dependent on specific solutions.

problem Dependence of the second fundamental form in local isometric immersions of pseudospherical surfaces.
method Analysis of third order differential equations and jets of finite order.
result The second fundamental form of pseudospherical surfaces is universal and not dependent on the specific solution.

TOLD++ improves convergence of diffusion models by critically damping the forward transition matrix.

problem Improving the convergence of Denoising Diffusion Probabilistic Models.
method Critically damping the Third-Order Langevin Dynamics (TOLD) forward transition matrix using eigen-analysis.
result TOLD++ converges faster than TOLD, verified on toy and real datasets.

Let VV be a vector space of dimension n+1n+1. We demonstrate that nn-component third-order Hamiltonian operators of differential-geometric type are parametrised by the algebraic variety of elements of rank nn in S2(Λ2V)S^2(Λ^2V) that lie in the kernel of the natural map S2(Λ2V)Λ4VS^2(Λ^2V)\to Λ^4V. Non-equivalent operators corres…

2015-08-11abs ↗pdf ↗

The paper bounds eigenvalues of specific operators on certain manifolds.

problem Bounding eigenvalues of Paneitz and third-order boundary operators on locally conformally flat manifolds.
method Proof based on conformal equivalence to canonical models, showing injectivity of developing maps, and explicit computations on canonical models.
result Eigenvalue bounds for the Paneitz operator and its associated third-order boundary operator on locally conformally flat manifolds.

We investigate nn-component systems of conservation laws that possess third-order Hamiltonian structures of differential-geometric type. The classification of such systems is reduced to the projective classification of linear congruences of lines in Pn+2\mathbb{P}^{n+2} satisfying additional geometric constraints. Algeb…

2017-03-17abs ↗pdf ↗

In this paper we define nnth order Hessian structures on manifolds and study them. In particular, when n=3n = 3, we make a detailed study and establish a one-to-one correspondence between {\it third-order Hessian structures} and a {\it certain class of connections} on the second-order tangent bundle of a manifold. Furt…

2005-08-25abs ↗pdf ↗

Third-order PDEs describe spherical and pseudospherical surfaces.

problem Equations for spherical and pseudospherical surfaces.
method Classification of third-order PDEs using compatibility conditions and linear problems.
result Explicit classification of equations describing spherical and pseudospherical surfaces.

The Cartan equivalence method is applied to provide an invariant characterization of the third-order ordinary differential equation u=f(x,u,u,u)u'''=f(x,u,u',u'') which admits a five-dimensional point symmetry Lie algebra. The invariant characterization is given in terms of the function ff in a compact form. A simple procedure …

2017-11-22abs ↗pdf ↗

In this sequel we extend the derivation of the third order helicity to magnetic fields supported on unlinked domains in 3-space. The formula is expressed in terms of generators of the deRham cohomology of the configuration space of three points in R3\R^3, which is a more practical domain from the perspective of applica…

2009-06-18abs ↗pdf ↗

New method computes affine normal directions efficiently for sparse polynomials.

problem Computing affine normal directions is computationally expensive in high dimensions.
method Reduces third-order tensor contraction to matrix-free formulation using log-determinant gradient.
result Scalable implementations with near-linear scaling in dimension and sparsity.

The paper studies steady motions of fibre-reinforced fluids on curved surfaces.

problem Analyzing steady motions of fibre-reinforced fluids on curved surfaces.
method Expressing kinematic equations in terms of the intrinsic Gauss equation and identifying integrable cases.
result Derives a variant of the integrable Tzitzéica equation encoding orthogonal coordinate systems on pseudospherical surfaces.

General Relativity in 4 dimensions can be equivalently described as a dynamical theory of SO(3)-connections rather than metrics. We introduce the notion of asymptotically hyperbolic connections, and work out an analog of the Fefferman-Graham expansion in the language of connections. As in the metric setup, one can solv…

2015-12-22abs ↗pdf ↗

The paper studies third-order PDEs invariant under affine transformations and connects them to the Fubini-Pick invariant.

problem Investigating third-order PDEs invariant under affine transformations.
method Using a general method introduced in [D.V. Alekseevsky, J. Gutt, G. Manno, and G. Moreno: A general method to construct invariant PDEs on homogeneous manifolds].
result Derives third-order PDEs from the Fubini-Pick invariant.

We present an elementary argument that one can shield linearised gravitational fields using linearised gravitational fields. This is done by using third-order potentials for the metric, which avoids the need to solve singular equations in shielding or gluing constructions for the linearised metric.

2017-01-02abs ↗pdf ↗