Articles
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10/09/2018--
10/09/2018
The seed order
We study various orders on countably complete ultrafilters on ordinals that
coincide and are wellorders under a hypothesis called the Ultrapower Axiom. Our
main focus is on the relationship between the Ultrapower Axiom and the
linearity of these orders.
Gabriel Goldberg
12/06/1994--
12/06/1994
Gaussian Fluctuation in Random Matrices
Let $N(L)$ be the number of eigenvalues, in an interval of length $L$, of a
matrix chosen at random from the Gaussian Orthogonal, Unitary or Symplectic
ensembles of ${\cal N}$ by ${\cal N}$ matrices, in the limit ${\cal
N}\rightarrow\infty$. We prove that $[N(L) - \langle N(L)\rangle]/\sqrt{\log
L}$ has a Gaussian distribution when $L\rightarrow\infty$. This theorem, which
requires control of all the higher moments of the distribution, elucidates
numerical and exact results on chaotic quantum systems and on the statistics of
zeros of the Riemann zeta function. \noindent PACS nos. 05.45.+b, 03.65.-w
Ovidiu Costin
Joel L. Lebowitz
10/24/2004--
10/24/2004
Dually degenerate varieties and the generalization of a theorem of Griffiths--Harris
The dual variety X* for a smooth n-dimensional variety X of the projective
space P^N is the set of tangent hyperplanes to X. In the general case, the
variety X* is a hypersurface in the dual space (P^N)*. If dim X* < N - 1, then
the variety X is called dually degenerate.
The authors refine these definitions for a variety X \subset P^N with a
degenerate Gauss map of rank r. For such a variety, in the general case, the
dimension of its dual variety X* is N - l - 1, where l = n - r, and X is dually
degenerate if dim X* < N - l - 1.
In 1979 Griffiths and Harris proved that a smooth variety X \subset P^N is
dually degenerate if and only if all its second fundamental forms are singular.
The authors generalize this theorem for a variety X \subset P^N with a
degenerate Gauss map of rank r.
Maks A. Akivis
Vladislav V. Goldberg
07/09/2020--
07/09/2020
Some combinatorial properties of Ultimate L and V
This paper establishes a number of constraints on the structure of large
cardinals under strong compactness assumptions. These constraints coincide with
those imposed by the Ultrapower Axiom, a principle that is expected to hold in
Woodin's hypothesized Ultimate \(L\), providing some evidence for the Ultimate
\(L\) Conjecture.
We show that every regular cardinal above the first strongly compact that
carries an indecomposable ultrafilter is measurable, answering a question of
Silver for large enough cardinals. We show that any successor almost strongly
compact cardinal of uncountable cofinality is strongly compact, making progress
on a question of Boney, Unger, and Brooke-Taylor. We show that if there is a
proper class of strongly compact cardinals then there is no nontrivial cardinal
preserving elementary embedding from the universe of sets into an inner model,
answering a question of Caicedo granting large cardinals. Finally, we show that
if \(\kappa\) is strongly compact, then \(V\) is a set forcing extension of the
inner model \(\kappa\text{-HOD}\) consisting of sets that are hereditarily
ordinal definable from a \(\kappa\)-complete ultrafilter over an ordinal;
\(\kappa\text{-HOD}\) seems to be the first nontrivial example of a ground of
\(V\) whose definition does not involve forcing.
Gabriel Goldberg
06/24/2024--
06/24/2024
Optimizing measurement tradeoffs in multiparameter spatial superresolution
The quantum Cram\'er-Rao bound for the joint estimation of the centroid and
the separation between two incoherent point sources cannot be saturated. As
such, the optimal measurements for extracting maximal information about both at
the same time are not known. In this work, we ascertain these optimal
measurements for an arbitrary point spread function, in the most relevant
regime of a small separation between the sources. Our measurement can be
adjusted within a set of tradeoffs, allowing more information to be extracted
from the separation or the centroid while ensuring that the total information
is the maximum possible.
J. Řeháček
J. L. Romero
A. Z. Goldberg
Z. Hradil
L. L. Sánchez-Soto
09/17/2008--
09/17/2008
Single source shortest paths in $H$-minor free graphs
We present an algorithm for the Single Source Shortest Paths (SSSP) problem
in \emph{$H$-minor free} graphs. For every fixed $H$, if $G$ is a graph with
$n$ vertices having integer edge lengths and $s$ is a designated source vertex
of $G$, the algorithm runs in $\tilde{O}(n^{\sqrt{11.5}-2} \log L) \le
O(n^{1.392} \log L)$ time, where $L$ is the absolute value of the smallest edge
length. The algorithm computes shortest paths and the distances from $s$ to all
vertices of the graph, or else provides a certificate that $G$ is not $H$-minor
free. Our result improves an earlier $O(n^{1.5} \log L)$ time algorithm for
this problem, which follows from a general SSSP algorithm of Goldberg.
Raphael Yuster
01/15/2024--
01/15/2024
Multipoles from Majorana constellations
Majorana stars, the $2S$ spin coherent states that are orthogonal to a
spin-$S$ state, offer an elegant method to visualize quantum states, disclosing
their intrinsic symmetries. These states are naturally described by the
corresponding multipoles. These quantities can be experimentally determined and
allow for an SU(2)-invariant analysis. We investigate the relationship between
Majorana constellations and state multipoles, thus providing insights into the
underlying symmetries of the system. We illustrate our approach with some
relevant and informative examples.
J. L. Romero
A. B. Klimov
A. Z. Goldberg
G. Leuchs
L. L. Sanchez-Soto
03/15/2002--
03/15/2002
The Goldberg-Sachs theorem in linearized gravity
The Goldberg-Sachs theorem has been very useful in constructing algebraically
special exact solutions of Einstein vacuum equation. Most of the physical
meaningful vacuum exact solutions are algebraically special. We show that the
Goldberg-Sachs theorem is not true in linearized gravity. This is a remarkable
result, which gives light on the understanding of the physical meaning of the
linearized solutions.
S. Dain
O. M. Moreschi
06/20/2009--
06/20/2009
Comparison of spaces of Hardy type for the Ornstein-Uhlenbeck operator
Denote by g the Gauss measure on R^n and by L the Ornstein-Uhlenbeck
operator. In this paper we introduce a local Hardy space h^1(g) of Goldberg
type and we compare it with the Hardy space H^1(g) introduced in a previous
paper by Mauceri and Meda. We show that for each each positive r the imaginary
powers of the operator rI+L are unbounded from h^1(g) to L^1(g). This result is
in sharp contrast both with the fact that the imaginary powers are bounded from
$H^1(g}$ to L^1(g), and with the fact that for the Euclidean laplacian \Delta
and the Lebesgue measure \lambda) the imaginary powers of rI-\Delta are bounded
from the Goldberg space h^1(\lambda) to L^1(\lambda). We consider also the case
of Riemannian manifolds M with Riemannian measure m. We prove that, under
certain geometric assumptions on M, an operator T, bounded on L^2(m), and with
a kernel satisfying certain analytic assumptions, is bounded from H^1(m) to
L^1(m) if and only if it is bounded from h^1(m) to L^1(m). Here H^1(m) denotes
the Hardy space on locally doubling metric measure spaces introduced by the
authors in arXiv:0808.0146, and h^1(m) is a Goldberg type Hardy space on M,
equivalent to a space recently introduced by M. Taylor. The case of translation
invariant operators on homogeneous trees is also considered.
A. Carbonaro
G. Mauceri
S. Meda
08/12/2021--
08/12/2021
Taming singularities of the quantum Fisher information
Quantum Fisher information matrices (QFIMs) are fundamental to estimation
theory: they encode the ultimate limit for the sensitivity with which a set of
parameters can be estimated using a given probe. Since the limit invokes the
inverse of a QFIM, an immediate question is what to do with singular QFIMs.
Moreover, the QFIM may be discontinuous, forcing one away from the paradigm of
regular statistical models. These questions of nonregular quantum statistical
models are present in both single- and multiparameter estimation.
Geometrically, singular QFIMs occur when the curvature of the metric vanishes
in one or more directions in the space of probability distributions, while
QFIMs have discontinuities when the density matrix has parameter-dependent
rank. We present a nuanced discussion of how to deal with each of these
scenarios, stressing the physical implications of singular QFIMs and the
ensuing ramifications for quantum metrology.
Aaron Z. Goldberg
José L. Romero
Ángel S. Sanz
Luis L. Sánchez-Soto
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