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<title>Physics - PhD Theses</title>
<link>http://hdl.handle.net/10468/430</link>
<description/>
<pubDate>Thu, 23 May 2013 23:16:52 GMT</pubDate>
<dc:date>2013-05-23T23:16:52Z</dc:date>
<item>
<title>Quantum behavior in mesoscopic systems</title>
<link>http://hdl.handle.net/10468/964</link>
<description>Quantum behavior in mesoscopic systems
Lo Gullo, Nicolino
In this thesis I present the work done during my PhD. The Thesis is divided into two parts; in the first one I present the study of mesoscopic quantum systems whereas in the second one I address the problem of the definition of Markov regime for quantum system dynamics. The first work presented is the study of vortex patterns in (quasi) two dimensional rotating Bose Einstein condensates (BECs). I consider the case of an anisotropy trapping potential and I shall show that the ground state of the system hosts vortex patterns that are unstable. In a second work I designed an experimental scheme to transfer entanglement from two entangled photons to two BECs. This work is meant to propose a feasible experimental set up to bring entanglement from microscopic to macroscopic systems for both the study of fundamental questions (quantum to classical transition) and technological applications. In the last work of the first part another experimental scheme is presented in order to detect coherences of a mechanical oscillator which is assumed to have been previously cooled down to the quantum regime. In this regime in fact the system can rapidly undergo decoherence so that new techniques have to be employed in order to detect and manipulate their states. In the scheme I propose a micro-mechanical oscillator is coupled to a BEC and the detection is performed by monitoring the BEC with a negligible back-action on the cantilever. In the second part of the thesis I give a definition of Markov regime for open quantum dynamics. The importance of such definition comes from both the mathematical description of the system dynamics and from the understanding of the role played by the environment in the evolution of an open system. In the Markov regime the mathematical description can be simplified and the role of the environment is a passive one.
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<pubDate>Tue, 01 Jan 2013 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://hdl.handle.net/10468/964</guid>
<dc:date>2013-01-01T00:00:00Z</dc:date>
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<title>Spatial and energetic mode dynamics of cold atomic systems</title>
<link>http://hdl.handle.net/10468/963</link>
<description>Spatial and energetic mode dynamics of cold atomic systems
O'Sullivan, Brian
In this thesis we relate the formal description of various cold atomic systems in the&#13;
energy eigenbasis, to the observable spatial mode dynamics. Herein the `spatial mode&#13;
dynamics' refers to the direction of photon emission following the spontaneous emission&#13;
of an excited fermion in the presence of a same species and spin ideal anisotropic Fermi&#13;
sea in its internal ground state. Due to the Pauli principle, the presence of the ground&#13;
state Fermi sea renders the phase space, anisotropic and only partially accessible, thereby&#13;
a ecting the direction of photon emission following spontaneous emission.&#13;
The spatial and energetic mode dynamics also refers to the quantum `tunneling' interaction&#13;
between localised spatial modes, synonymous with double well type potentials.&#13;
Here we relate the dynamics of the wavefunction in both the energetic and spatial representations.&#13;
Using this approach we approximate the relationship between the spatial&#13;
and energetic representations of a wavefunction spanning three spatial and energetic&#13;
modes. This is extended to a process known as Spatial Adiabatic Passage, which is a&#13;
technique to transport matter waves between localised spatial modes. This approach&#13;
allows us to interpret the transport of matter waves as a signature of a geometric phase&#13;
acquired by the one of the internal energy eigenstates of the system during the cyclical&#13;
evolution. We further show that this geometric phase may be used to create spatial&#13;
mode qubit and qutrit states.
</description>
<pubDate>Sat, 01 Dec 2012 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://hdl.handle.net/10468/963</guid>
<dc:date>2012-12-01T00:00:00Z</dc:date>
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<item>
<title>Tropospheric aerosol detection over Southern Ireland using a backscatter Raman lidar</title>
<link>http://hdl.handle.net/10468/996</link>
<description>Tropospheric aerosol detection over Southern Ireland using a backscatter Raman lidar
McAuliffe, Michael A. P.
Lidar is an optical remote sensing instrument that can measure atmospheric parameters. A Raman lidar instrument (UCLID) was established at University College Cork to contribute to the European lidar network, EARLINET. System performance tests were carried out to ensure strict data quality assurance for submission to the EARLINET database. Procedures include: overlap correction, telecover test, Rayleigh test and zero bin test. Raman backscatter coefficients, extinction coefficients and lidar ratio were measured from April 2010 to May 2011 and February 2012 to June 2012. Statistical analysis of the profiles over these periods provided new information about the typical atmospheric scenarios over Southern Ireland in terms of aerosol load in the lower troposphere, the planetary boundary layer (PBL) height, aerosol optical density (AOD) at 532 nm and lidar ratio values. The arithmetic average of the PBL height was found to be 608 ± 138 m with a median of 615 m, while average AOD at 532 nm for clean marine air masses was 0.119 ± 0.023 and for polluted air masses was 0.170 ± 0.036. The lidar ratio showed a seasonal dependence with lower values found in winter and autumn (20 ± 5 sr) and higher during spring and winter (30 ± 12 sr). Detection of volcanic particles from the eruption of the volcano Eyjafjallajökull in Iceland was measured between 21 April and 7 May 2010. The backscatter coefficient of the ash layer varied between 2.5 Mm-1sr-1 and 3.5 Mm-1sr-1, and estimation of the AOD at 532 nm was found to be between 0.090 and 0.215. Several aerosol loads due to Saharan dust particles were detected in Spring 2011 and 2012. Lidar ratio of the dust layers were determine to be between 45 and 77 sr and AOD at 532 nm during the dust events range between 0.84 to 0.494.
</description>
<pubDate>Sat, 01 Dec 2012 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://hdl.handle.net/10468/996</guid>
<dc:date>2012-12-01T00:00:00Z</dc:date>
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<title>Axial symmetry and transverse trace-free tensors in numerical relativity</title>
<link>http://hdl.handle.net/10468/527</link>
<description>Axial symmetry and transverse trace-free tensors in numerical relativity
Conboye, Rory P. A.
Transverse trace-free (TT) tensors play an important role in the initial conditions of numerical relativity, containing two of the component freedoms. Expressing a TT tensor entirely, by the choice of two scalar potentials, is not a trivial task however. Assuming the added condition of axial symmetry, expressions are given in both spherical and cylindrical coordinates, for TT tensors in flat space. A coordinate relation is then calculated between the scalar potentials of each coordinate system. This is extended to a non-flat space, though only one potential is found. The remaining equations are reduced to form a second order partial differential equation in two of the tensor components. With the axially symmetric flat space tensors, the choice of potentials giving Bowen-York conformal curvatures, are derived. A restriction is found for the potentials which ensure an axially symmetric TT tensor, which is regular at the origin, and conditions on the potentials, which give an axially symmetric TT tensor with a spherically symmetric scalar product, are also derived. A comparison is made of the extrinsic curvatures of the exact Kerr solution and numerical Bowen-York solution for axially symmetric black hole space-times. The Brill wave, believed to act as the difference between the Kerr and Bowen-York space-times, is also studied, with an approximate numerical solution found for a mass-factor, under different amplitudes of the metric.
</description>
<pubDate>Wed, 01 Feb 2012 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://hdl.handle.net/10468/527</guid>
<dc:date>2012-02-01T00:00:00Z</dc:date>
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