<?xml version="1.0" encoding="UTF-8"?>
<feed xmlns="http://www.w3.org/2005/Atom" xmlns:dc="http://purl.org/dc/elements/1.1/">
  <title>OAR@UM Collection:</title>
  <link rel="alternate" href="https://www.um.edu.mt/library/oar/handle/123456789/10990" />
  <subtitle />
  <id>https://www.um.edu.mt/library/oar/handle/123456789/10990</id>
  <updated>2026-04-11T14:24:23Z</updated>
  <dc:date>2026-04-11T14:24:23Z</dc:date>
  <entry>
    <title>An integrated system for telescope control using FPGA(s)</title>
    <link rel="alternate" href="https://www.um.edu.mt/library/oar/handle/123456789/91635" />
    <author>
      <name />
    </author>
    <id>https://www.um.edu.mt/library/oar/handle/123456789/91635</id>
    <updated>2022-03-17T10:54:17Z</updated>
    <published>2016-01-01T00:00:00Z</published>
    <summary type="text">Title: An integrated system for telescope control using FPGA(s)
Abstract: Astronomical radio interferometers typically consist of an array of antennas, widely separated and connected using a transmission line. Signals recorded from each antenna are sent to a back-end where they are digitised, channelised and superposed, giving rise to constructive / destructive interference depending on their phase difference. This technique of interferometry is called aperture synthesis and it results in a combined telescope with a resolution equivalent to that of a single antenna with a diameter equal to the spacing of the antennas furthest apart in the array. When we consider a radio signal from a celestial source, incident on two antennas separated by a distance, the antennas receive the radio signal with a time difference, causing the signals to be out of phase. In order to achieve power amplification, the recorded signals must be phased using a technique called beamforming. A beamformer, has the added capability of steering the beam of a radio telescope using constructive / destructive interference. &#xD;
The aim of this project was to design and implement an integrated control system (ICS) for the digital steering of beams in a radio telescope. The system design was based on the PAPER F-engine and implemented on the ROACH2 FPGA board. A beamformer module was designed using the CASPER XPS tool-flow to be capable of continually steering beams in the sky, whilst monitoring the behaviour of a phased array system to ensure that the beams are continually tracking a source.
Description: B.SC.(HONS)MATHS&amp;PHYSICS</summary>
    <dc:date>2016-01-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Σ-hypergraphs : colouring, independence, matchings and hamiltonicity</title>
    <link rel="alternate" href="https://www.um.edu.mt/library/oar/handle/123456789/13461" />
    <author>
      <name />
    </author>
    <id>https://www.um.edu.mt/library/oar/handle/123456789/13461</id>
    <updated>2018-06-27T06:26:05Z</updated>
    <published>2016-01-01T00:00:00Z</published>
    <summary type="text">Title: Σ-hypergraphs : colouring, independence, matchings and hamiltonicity
Abstract: A hypergraph H is a  nite set V (H) of vertices together with a family E(H) of&#xD;
subsets of V (H) called hyperedges (or simply edges). An r-uniform hypergraph&#xD;
is one in which all the edges are of the same size r. So a standard graph can be&#xD;
defined as a 2-uniform hypergraph.&#xD;
Hypergraphs arose naturally as an extension to graphs, with the main intent&#xD;
of extending important and interesting results from Graph Theory to this generalised&#xD;
setting. The results were sometimes simplified, and in other instances&#xD;
unexpected.&#xD;
In this thesis we study various properties of a special family of hypergraphs,&#xD;
the  -hypergraphs, a generalisation of  -hypergraphs,  first defined by Caro&#xD;
and Lauri and studied in the context of Voloshin colourings, focusing mainly&#xD;
on non-monochromatic-non-rainbow (NMNR) colourings. The most interesting&#xD;
aspect of these types of colourings is arguably the appearance of gaps in&#xD;
the chromatic spectrum of the hypergraph. Results in this area of study often&#xD;
required ad-hoc and complex hypergraph structures such as designs. Both  -&#xD;
and  -hypergraphs proved to be a simple unifying construction in this respect&#xD;
giving interesting results and chromatic spectra by controlling the parameters&#xD;
which define the structure. Furthermore, they also proved to have interesting&#xD;
properties with respect to other hypergraph theoretic properties such as&#xD;
independence, matchings and Hamiltonicity, as we shall see in this thesis.
Description: PH.D.MATHS</summary>
    <dc:date>2016-01-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>On the spectra and walks of molecular and controllable graphs</title>
    <link rel="alternate" href="https://www.um.edu.mt/library/oar/handle/123456789/13460" />
    <author>
      <name />
    </author>
    <id>https://www.um.edu.mt/library/oar/handle/123456789/13460</id>
    <updated>2018-06-27T06:35:45Z</updated>
    <published>2016-01-01T00:00:00Z</published>
    <summary type="text">Title: On the spectra and walks of molecular and controllable graphs
Abstract: Walks in a graph G relate to its configuration and to the eigenspaces of its adjacency&#xD;
matrix G. In this thesis, we extend the notion of walks. It impacts on the inverse&#xD;
of G, settling a conjecture on the conductivity properties of molecules modelled by&#xD;
chemical graphs, whose vertices represent carbon atoms having degree at most three.&#xD;
Walks also bring out structural properties of a controllable system represented by G.&#xD;
The product of the weights of the edges  in a walk of length on a weighted&#xD;
looped graph G is called the walk weight. We deduce closed form expressions for&#xD;
the generating function of the sum of walk weights of G between vertices among&#xD;
two subsets of the vertices of G. We produce three expressions for this generating&#xD;
function: one in terms of the eigenvalues and eigenspaces of G, one in terms of the&#xD;
inverse of the matrix, where I is the identity matrix, and one in terms of&#xD;
the characteristic polynomials of G and those of related graphs, called overgraphs,&#xD;
obtained from G by adding a vertex. In the latter case, characteristic polynomials&#xD;
with a reversal of their coefficients, called reverse polynomials, are employed. We&#xD;
introduce the notion of a walk of negative length on the graph G as being a walk on&#xD;
the weighted looped graph whose adjacency matrix is the inverse of that of G. Similar&#xD;
to the case for the usual, positively{long walks, we provide generating functions&#xD;
producing sums of walk weights of negative length, and relate these walk weight&#xD;
sums with those of positive length. Remarkably, if we use characteristic polynomials&#xD;
to produce generating functions of the sum of the weights of walks of negative lengths,&#xD;
the usual characteristic polynomials are used, rather than their reversal as in the case&#xD;
for positively long walks.&#xD;
In the literature, the walk matrix of a graph G is a square matrix whose ijth entry&#xD;
is the number of walks of length between vertex j and any other vertex of G.&#xD;
We extend this notion to walk matrices whose entries represent walks between each&#xD;
vertex and a subset of the vertex set of G. Hankel matrices whose entries enumerate&#xD;
walk weights of a graph are also discussed. They turn out to be Gram matrices of the&#xD;
columns of the walk matrix of the graph. Another matrix in the form of a Toeplitz&#xD;
matrix, combining walks of both positive and negative length, is also introduced. A&#xD;
new walk matrix that mimics the properties of the commonly used walk matrix, but&#xD;
containing the sum of walk weights of closed walks in G instead of the number of walks, is also proposed. Our study of properties revealed in walk matrices contributes&#xD;
to new discoveries in molecular chemistry and in control theory.
Description: PH.D.MATHS</summary>
    <dc:date>2016-01-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Two-fold isomorphisms</title>
    <link rel="alternate" href="https://www.um.edu.mt/library/oar/handle/123456789/10995" />
    <author>
      <name />
    </author>
    <id>https://www.um.edu.mt/library/oar/handle/123456789/10995</id>
    <updated>2018-06-27T06:55:37Z</updated>
    <published>2016-01-01T00:00:00Z</published>
    <summary type="text">Title: Two-fold isomorphisms
Abstract: In this dissertation, we present a natural generalization of the notion of isomorphism of a&#xD;
graph or digraph G, namely two-fold isomorphisms from a graph or digraph G to a graph&#xD;
or digraph H.&#xD;
A mixed graph is a pair G = (V (G),A(G)) where V (G) is a finite set and A(G) is a set&#xD;
of ordered pairs of elements of V (G). The elements of V (G) are called vertices and the&#xD;
elements of A(G) are called arcs. When referring to an arc (u, v), we say that u is adjacent&#xD;
to v and v is adjacent from u. The vertex u is the tail and v is the head of a given arc&#xD;
(u, v). An arc of the form (u, u) is a loop. A mixed graph cannot contain multiple arcs,&#xD;
that is, it cannot contain the arc (u, v) more than once. A set S of arcs is self-paired if,&#xD;
whenever (u, v) 2 S, (v, u) is also in S. If S = {(u, v), then(v, u)}, then we identify S with&#xD;
the unordered pair {u, v}; this unordered pair is called an edge.&#xD;
It will be useful to consider two special cases of mixed graphs. An undirected graph or, in&#xD;
short graph, is a mixed graph without loops whose arc-set is self-paired. The edge set of a&#xD;
graph is denoted by E(G). A digraph is a mixed graph with no loops in which no arc is&#xD;
self-paired.&#xD;
A two-fold isomorphism (TF-isomorphism) is a pair (α, β) of permutations of the vertex set&#xD;
V (G) which acts on ordered pairs of vertices of G in the natural way and such that (u, v) is&#xD;
an arc in G if and only if (α(u), β(v)) is also an arc in H. When α = β the TF-isomorphism&#xD;
is just a usual isomorphism.&#xD;
The following is a brief outline of this dissertation.&#xD;
Chapter 1: In this chapter, we define canonical double covers, incidence double covers&#xD;
and alternating double covers. We also define alternating trails or A-trails. Furthermore,&#xD;
we introduce the notion of stability of graphs. In later chapters, seemingly unrelated concepts&#xD;
and ideas are brought together through the concept of two-fold isomorphism.&#xD;
Chapter 2: As far as we know, TF-isomorphisms of graphs were first introduced by Zelinka&#xD;
[35, 36] who was motivated by the study of isotopy of groupoids, referring to what we call&#xD;
‘TF-automorphisms’ as ‘autotopies’. Zelinka’s work had been overlooked for decades. Here&#xD;
we review the early work by Zelinka [34, 35, 36, 37, 38], Porcu [26], Pacco and Scapellato&#xD;
[24], and Maruˇsiˇc, Scapellato and Zagaglia-Salvi [21, 22] which, in hindsight, involved TFisomorphisms.&#xD;
Chapter 3: In this chapter we start developing material to tackle our problems. We start&#xD;
by addressing questions concerning invariance under TF-isomorphisms. Then we use alternating&#xD;
double covers of graphs to be able to extend certain results previously known&#xD;
to hold for graphs to mixed graphs. We conclude this chapter by defining an equivalence&#xD;
relation on the arc-set of any mixed graph G and bringing together the concept of A-trails&#xD;
and the construction of graph covers to ultimately explain how TF-isomorphisms arise.&#xD;
Chapter 4: In this chapter, we use and develop new theory with the aim of constructing&#xD;
graphs with specific properties. In particular, we are interested in asymmetric graphs which&#xD;
have a non-trivial TF-automorphism group. We construct a smallest unstable graph using&#xD;
two different constructions, one of which will be generalized in Chapter 5. We also show&#xD;
that a graph and a digraph can be TF-isomorphic. Chapter 5: In this chapter, we show how TF-isomorphisms provide a fresh outlook when&#xD;
considering the concept of unstable graphs. We first show that there is a link between&#xD;
TF-automorphisms and graph stability. We then present simple arguments concerning triangles&#xD;
to ultimately present a method for constructing unstable graphs of arbitrarily large&#xD;
diameter. We also generalize one of the methods used to construct a smallest asymmetric&#xD;
unstable graph and asymmetric unstable graphs of arbitrarily large instability index.&#xD;
Chapter 6: In this chapter, we look at TF-orbitals in some more detail. We define the&#xD;
TF-rank of a group of TF-permutations and look at the situation where the TF-rank equals&#xD;
1 or 2. We then apply this to unstable rank 3 strongly regular graphs. We consider further&#xD;
properties on a TF-permutation group which force the TF-orbitals to satisfy structure constants&#xD;
similar to those of a coherent configuration.&#xD;
Chapter 7: In the final chapter, we review in a little more detail the connection between&#xD;
TF-isomorphisms and problems such as the Neighbourhood Reconstruction Problem. We&#xD;
also discuss a method suggested by Klin to extend the notion of stability to digraphs and&#xD;
finally we reveal new avenues for research which we plan to explore in the near future.&#xD;
Chapter 1 and Chapter 3 include results found in [16, 17, 18]. Chapter 4 includes constructions&#xD;
found in [16]. Most of the contents of Chapter 5 appear in [18], whereas the contents of&#xD;
Chapter 6 are included in a paper which at the time of writing has been accepted for publication&#xD;
in the Journal of Combinatorial Mathematics and Combinatorial Computing. At&#xD;
the time of writing, a paper which describes the construction of a smallest unstable graph&#xD;
and of a family of graphs with an arbitrarily large index of stability is being prepared.&#xD;
These constructions are found in Chapter 4 and Chapter 5 respectively.
Description: PH.D.MATHS</summary>
    <dc:date>2016-01-01T00:00:00Z</dc:date>
  </entry>
</feed>

