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As noted in the Introduction, in this chapter we consider running the Toda algorithm only until time , the deflation time with block decomposition k = 1 fixed, when the norm of the off-diagonal elements in the first row, and hence the first column, is . Define so that if then is an eigenvalue of H. Thus, with as in (6.1), the halting time (or 1-deflation time) for the Toda algorithm is given by .
There are still algebraic surprises lying concealed within the Toda flow that we have not yet described. A simple argument with matrix factorizations gives rise to new inverse variables, the Z-coordinates, together with new commuting vector fields. In these new variables, the Toda flows become explicit, straight line motions in for an appropriate dimension N (Toda flows on full matrices are also considered). Moreover, orbit limits, such as diagonal matrices, lie beyond the scope of standard variables (see, e.g., M below for Jacobi matrices), and the asymptotic analysis must proceed using ad hoc methods. Such orbit limits, however, belong to the domain of the new variables, and asymptotic computations are easily performed through local theory. As described in Remark 4.14, the methods in this section extend the purview of the Toda system substantially.
The goal of this chapter is to give an elementary introduction to Hamiltonian mechanics, and particularly integrable Hamiltonian systems, with a view to describing various results that we need in analyzing the Toda algorithm. The reader is encouraged to consult references such as Abraham and Marsden (1978), Arnold (1978), Kirillov (2004), Moser and Zehnder (2005) and Warner (1983) for a more detailed presentation.
We now turn to studying the Toda lattice. As noted in Chapter 1, the (open) Toda lattice was introduced by H. Toda in 1967 and describes the motion of N particles on the real line, generated by the Hamiltonian on the symplectic manifold .
We now introduce the results from random matrix theory that are needed to prove Theorem 6.2 and Proposition 6.5 in the next chapter.Let H be an N x N Hermitian (or real symmetric) matrix with eigenvalues and let denote the absolute value of the first components of the normalized eigenvectors.We assume the entries of H are distributed according to an invariant or generalized Wigner ensemble (see Section 5.1).
Our main goal is to prove the result of Deift and Trogdon (2018) on universality for the Toda eigenvalue algorithm to compute the top eigenvalue of a random real symmetric or Hermitian matrix H chosen from some random matrix ensemble. We concentrate first on the real symmetric case: The modifications that are necessary in the Hermitian case are given in Section 3.10.
In this paper, we consider a Hénon-type equation for the Grushin operator. After proving a radial lemma, we establish the existence of a solution for a superlinear and supercritical problem. Additionally, we derive a symmetry-breaking result for ground-state solutions in the subcritical case.
for piecewise constant functions $f$ with nonzero and zero values alternating. The above inequality strengthens a recent result of Bilz and Weigt [3] proved for indicator functions of bounded variation vanishing at $\pm\infty$. We conjecture that the inequality holds for all functions of bounded variation, representing a stronger version of the existing conjecture ${\rm Var} (Mf)\le {\rm Var} (f)$. We also obtain the discrete counterpart of our theorem, moreover proving a transference result on equivalency between both settings that is of independent interest.
Commutator blueprints can be seen as blueprints for constructing RGD systems over $\mathbb {F}_2$ with prescribed commutation relations. In this paper, we construct several families of Weyl-invariant commutator blueprints, mostly of universal type. Also applying another result of the author, we obtain new examples of exotic RGD systems of universal type over $\mathbb {F}_2$. In particular, we generalize Tits’ construction of uncountably many trivalent Moufang twin trees to higher rank, we obtain an example of an RGD system of rank $3$ such that the nilpotency degree of the groups $U_w$ is unbounded, and we construct a commutator blueprint of type $(4, 4, 4)$ that is used to answer a question of Tits from the late $1980$s about twin buildings.
where $2_{s}^{*}=\frac{2N}{N-2s}$, $s\in(\frac{1}{2},1)$, $N \gt 2s$, Ω is a bounded domain in $\mathbb{R}^N$, ɛ is a small parameter, and the boundary Σ is given in different ways according to the different definitions of the fractional Laplacian operator $(-\Delta)^{s}$. The operator $(-\Delta)^{s}$ is defined in two types: the spectral fractional Laplacian and the restricted fractional Laplacian. For the spectral case, Σ stands for $\partial \Omega$; for the restricted case, Σ is $\mathbb{R}^{N}\setminus \Omega$. Firstly, we provide a positive confirmation of the fractional Brezis–Peletier conjecture, that is, the above almost critical problem has a single bubbling solution concentrating around the non-degenerate critical point of the Robin function. Furthermore, the non-degeneracy andlocal uniqueness of this bubbling solution are established.
Let M be an open Riemann surface and $n\ge 3$ be an integer. In this paper, we establish some generic properties (in Baire category sense) in the space of all conformal minimal immersions $M\to{\mathbb{R}}^n$ endowed with the compact-open topology, pointing out that a generic such immersion is chaotic in many ways. For instance, we show that a generic conformal minimal immersion $u\colon M\to {\mathbb{R}}^n$ is non-proper, almost proper, and ${\mathfrak{g}}$-complete with respect to any given Riemannian metric ${\mathfrak{g}}$ in ${\mathbb{R}}^n$. Further, its image u(M) is dense in ${\mathbb{R}}^n$ and disjoint from ${\mathbb{Q}}^3\times {\mathbb{R}}^{n-3}$, and has infinite area, infinite total curvature, and unbounded curvature on every open set in ${\mathbb{R}}^n$. In case n = 3, we also prove that a generic conformal minimal immersion $M\to {\mathbb{R}}^3$ has infinite index of stability on every open set in ${\mathbb{R}}^3$.
We derive faithful inclusions of C*-algebras from a coend-type construction in unitary tensor categories. This gives rise to different potential notions of discreteness for an inclusion in the non-irreducible case and provides a unified framework that encloses the theory of compact quantum group actions. We also provide examples coming from semi-circular systems and from factorization homology. In the irreducible case, we establish conditions under which the C*-discrete and W*-discrete conditions are equivalent.