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A Comparison of Four Numerical Methods of Finding the Zeros of Real Polynomial EquationsPeterson, Robert Grant January 1966 (has links)
No description available.
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Numerical Method for Solving Higher Degree Polynomials for All Zeros in the Real and Complex DomainTaylor, S. C. January 1966 (has links)
No description available.
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Irreducibility of polynomials.Mahatabuddin, Mohammad January 1964 (has links)
No description available.
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Inequalities with orthogonal polynomialsRoosenraad, Cris Thomas, January 1969 (has links)
Thesis (Ph. D.)--University of Wisconsin--Madison, 1969. / Vita. Typescript. eContent provider-neutral record in process. Description based on print version record. Includes bibliographical references.
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Approximation theory for exponential weights.Kubayi, David Giyani. January 1998 (has links)
Much of weighted polynomial approximation originated with the famous
Bernstein qualitative approximation problem of 1910/11. The classical Bernstein
approximation problem seeks conditions on the weight functions \V
such that the set of functions {W(x)Xn};;"=l is fundamental in the class of
suitably weighted continuous functions on R, vanishing at infinity. Many
people worked on the problem for at least 40 years. Here we present a
short survey of techniques and methods used to prove Markov and Bernstein
inequalities as they underlie much of weighted polynomial approximation.
Thereafter, we survey classical techniques used to prove Jackson theorems
in the unweighted setting. But first we start, by reviewing some elementary
facts about orthogonal polynomials and the corresponding weight function
on the real line. Finally we look at one of the processes (If approximation,
the Lagrange interpolation and present the most recent results concerning
mean convergence of Lagrange interpolation for Freud and Erdos weights. / Andrew Chakane 2018
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Collective field theory of schur polynomialsSmith, Stephanie 07 October 2011 (has links)
MSc., Faculty of Science, University of the Witwatersrand, 2011 / We try to develop a collective field theory of single matrix models by using
the formalism of Jevicki and Sakita in [1], with Schur polynomials as our
collective fields. Field operators and the relation for the change of variables
required to obtain the collective field Hamiltonian are found using group
representation theory.
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The distinguished guests of giantsMathwin, Christopher Richard January 2016 (has links)
A thesis submitted to the Faculty of Science, University of the Witwatersrand, Johannesburg, in fulfilment of the requirements for the degree of Doctor of Philosophy. Johannesburg, 2016. / The convenient pictorial descriptions of the half-BPS and near-BPS sectors of the AdS=CFT equivalent
theories of N = 4, D = 4 super Yang-Mills and D = 10 Type IIB superstring theory on AdS5 S5 are
exploited in this thesis by using Schur polynomials labelled by Young diagrams as a basis for the gauge
invariant operators in the eld theory.
We use a \Fourier transform" on these operators to construct asymptotic eigenstates of the dilatation
operator, the spectrum of which agrees precisely with the rst two leading order terms in the smallcoupling
expansion of the exact result determined by symmetry. Motivated by the geometric description
of the systems of open strings with magnon excitations to which the operators are dual, we propose
a simple and minimal all-loop expression that interpolates between anomalous dimensions computed
in the gauge theory and energies computed in the string theory. The connection to the string theory
result provides the insight necessary to understand the interpretation of our Gauss graphs in the magnon
language. Symmetry determines the two-body scattering matrix for the magnons up to a phase, and it
is demonstrated that integrability is spoiled by the boundary conditions on the open strings.
The Schur polynomial construction is then applied to the study of closed strings on a class of half-
BPS excitations of the AdS5 S5 background. The string theory predictions for the magnon energies
are again reproduced by calculating the anomalous dimensions of particular linear combinations of our
operators. Group theoretic quantities which can be read o the Young diagram labels provide the correct
modi cation of terms in the dilatation action to account for the energies of magnons at di erent radii on
the LLM plane. The representation theory implies a natural splitting of the full symmetry group - the
distinction between what is the background and what is the excitation is accomplished in the choice of
the subgroup and representations used to construct the operator.
Connecting the descriptions utilised in obtaining these results is expected to allow the construction of
operators dual to general open string con gurations on the class of backgrounds considered. / GR 2016
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When does a Submodule of (R[x$_1$,$ldots$, x$_k$])$^n$ Contain a Positive Element?21 May 2001 (has links)
No description available.
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Explicit Factorization of Generalized Cyclotomic Polynomials of Order $2^m 3$ Over a Finite Field $F_q$Tosun, Cemile 01 August 2013 (has links)
We give explicit factorizations of $a$-cyclotomic polynomials of order $2^m 3$, $Q_{2^m3,a}(x)$, over a finite field $F_q$ with $q$ elements where $q$ is a prime power, $m$ is a nonnegative integer and $a$ is a nonnegative element of $F_q$. We use the relation between usual cyclotomic polynomials and $a$-cyclotomic polynomials. Factorizations split into eight categories according to $q \equiv \pm1$ (mod 4), $a$ and $-3$ are square in $F_q$. We find that the coefficients of irreducible factors are primitive roots of unity and in some cases that are related with Dickson polynomials.
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Some problems in knot theoryKeever, Robert Dudley January 1989 (has links)
No description available.
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