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  <channel rdf:about="https://www.um.edu.mt/library/oar/handle/123456789/2065">
    <title>OAR@UM Collection:</title>
    <link>https://www.um.edu.mt/library/oar/handle/123456789/2065</link>
    <description />
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        <rdf:li rdf:resource="https://www.um.edu.mt/library/oar/handle/123456789/146592" />
        <rdf:li rdf:resource="https://www.um.edu.mt/library/oar/handle/123456789/146398" />
        <rdf:li rdf:resource="https://www.um.edu.mt/library/oar/handle/123456789/145823" />
        <rdf:li rdf:resource="https://www.um.edu.mt/library/oar/handle/123456789/142655" />
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    <dc:date>2026-05-27T21:53:07Z</dc:date>
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  <item rdf:about="https://www.um.edu.mt/library/oar/handle/123456789/146592">
    <title>The JWST hubble sequence : the rest-frame optical evolution of galaxy structure at 1.5&lt;z&lt;6.5</title>
    <link>https://www.um.edu.mt/library/oar/handle/123456789/146592</link>
    <description>Title: The JWST hubble sequence : the rest-frame optical evolution of galaxy structure at 1.5&lt;z&lt;6.5
Authors: Ferreira, Leonardo; Conselice, Christopher J.; Sazonova, Elizaveta; Ferrari, Fabricio; Caruana, Joseph; Tohill, Clár-Bríd; Lucatelli, Geferson; Adams, Nathan; Irodotou, Dimitrios; Marshall, Madeline A.; Roper, Will J.; Lovell, Christopher C.; Verma, Aprajita; Austin, Duncan; Trussler, James; Wilkins, Stephen M.
Abstract: We present results on the morphological and structural evolution of a total of 3956 galaxies observed with JWST at 1.5 &lt; z &lt; 6.5 in the JWST CEERS observations that overlap with the CANDELS EGS field. This is the biggest visually classified sample observed with JWST yet, ∼20 times larger than previous studies, and allows us to examine in detail how galaxy structure has changed over this critical epoch. All sources were classified by six individual classifiers using a simple classification scheme aimed at producing disk/spheroid/peculiar classifications, whereby we determine how the relative number of these morphologies has evolved since the Universe’s first billion years. Additionally, we explore structural and quantitative morphology measurements using Morfometryka, and show that galaxies with M* &gt; 109 M⊙ at z &gt; 3 are not dominated by irregular and peculiar structures, either visually or quantitatively, as previously thought. We find a strong dominance of morphologically selected disk galaxies up to z = 6 in this mass range. We also find that the stellar mass and star formation rate densities are dominated by disk galaxies up to z ∼ 6, demonstrating that most stars in the Universe were likely formed in a disk galaxy. We compare our results to theory to show that the fraction of types we find is predicted by cosmological simulations, and that the Hubble Sequence was already in place as early as one billion years after the Big Bang. Additionally, we make our visual classifications public for the community.</description>
    <dc:date>2023-01-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="https://www.um.edu.mt/library/oar/handle/123456789/146398">
    <title>Variational Gibbs state preparation on NISQ devices</title>
    <link>https://www.um.edu.mt/library/oar/handle/123456789/146398</link>
    <description>Title: Variational Gibbs state preparation on NISQ devices
Abstract: The preparation of an equilibrium thermal state of a quantum many-body system on noisy intermediate-scale quantum (NISQ) devices is an important task in order to extend the range of applications of quantum computation. Faithful Gibbs state preparation would pave the way to investigate protocols such as thermalization and out-of-equilibrium thermodynamics, as well as providing useful resources for quantum algorithms, where sampling from Gibbs states constitutes a key subroutine. We propose a variational quantum algorithm (VQA) to prepare Gibbs states of a quantum many-body system. The novelty of our VQA consists in implementing a parameterized quantum circuit acting on two distinct, yet connected (via CNOT gates), quantum registers. The VQA evaluates the Helmholtz free energy, where the von Neumann entropy is obtained via post-processing of computational basis measurements on one register, while the Gibbs state is prepared on the other register, via a unitary rotation in the energy basis. Finally, we benchmark our VQA by preparing Gibbs states of the transverse field Ising and Heisenberg XXZ models and achieve remarkably high fidelities across a broad range of temperatures in statevector simulations. We also assess the performance of the VQA on IBM quantum computers, showcasing its feasibility on current NISQ devices.</description>
    <dc:date>2023-01-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="https://www.um.edu.mt/library/oar/handle/123456789/145823">
    <title>EPOCHS VI : the size and shape evolution of galaxies since z ∼8 with JWST observations</title>
    <link>https://www.um.edu.mt/library/oar/handle/123456789/145823</link>
    <description>Title: EPOCHS VI : the size and shape evolution of galaxies since z ∼8 with JWST observations
Authors: Ormerod, Katherine; Conselice, Christopher J.; Adams, Nathan J.; Harvey, Thomas A.; Austin, Duncan; Trussler, James A.A.; Ferreira, Leonardo De Albernaz; Caruana, Joseph; Lucatelli, Geferson; Li, Qiong; Roper, William J.
Abstract: We present the results of a size and structural analysis of 1395 galaxies at 0.5 ≤ z ≲ 8 with stellar masses log (M*/M⊙)&gt; 9.5 within the James Webb Space Telescope Public CEERS field that overlaps with the Hubble Space Telescope Cosmic Assembly Near-infrared Deep Extragalactic Legacy Survey EGS observations. We use GALFIT to fit single Sérsic models to the rest-frame optical profile of our galaxies, which is a mass-selected sample complete to our redshift and mass limit. Our primary result is that at fixed rest-frame wavelength and stellar mass, galaxies get progressively smaller, evolving as ∼(1 + z)−0.71 ± 0.19 up to z ∼ 8. We discover that the vast majority of massive galaxies at high redshifts have low Sérsic indices, thus do not contain steep, concentrated light profiles. Additionally, we explore the evolution of the size–stellar mass relationship, finding a correlation such that more massive systems are larger up to z ∼ 3. This relationship breaks down at z &gt; 3, where we find that galaxies are of similar sizes, regardless of their star formation rates and Sérsic index, varying little with mass. We show that galaxies are more compact at redder wavelengths, independent of sSFR or stellar mass up to z ∼ 3. We demonstrate the size evolution of galaxies continues up to z ∼ 8, showing that the process or causes for this evolution is active at early times. We discuss these results in terms of ideas behind galaxy formation and evolution at early epochs, such as their importance in tracing processes driving size evolution, including minor mergers and active galactic nuclei activity.</description>
    <dc:date>2024-01-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="https://www.um.edu.mt/library/oar/handle/123456789/142655">
    <title>The interplay between accretion, downsizing, and the formation of box/peanut bulges in TNG50</title>
    <link>https://www.um.edu.mt/library/oar/handle/123456789/142655</link>
    <description>Title: The interplay between accretion, downsizing, and the formation of box/peanut bulges in TNG50
Authors: Anderson, Stuart Robert; Gough-Kelly, Steven; Debattista, Victor P.; Du, Min; Erwin, Peter; Cuomo, Virginia; Caruana, Joseph; Hernquist, Lars; Vogelsberger, Mark
Abstract: From the TNG50 cosmological simulation we build a sample of 191 well-resolved barred galaxies with stellar mass&#xD;
log(M/M) &gt; 10 at z = 0. We search for box/peanut bulges (BPs) in this sample, finding them in 55 per cent of cases.&#xD;
We compute fBP, the BP probability for barred galaxies as a function of M, and find that this rises to a plateau, as found in&#xD;
observations of nearby galaxies. The transition mass where fBP reaches half the plateau value is log(M/M) = 10.13 ± 0.07,&#xD;
consistent with the observational value within measurement errors. We show that this transition in fBP can be attributed to the&#xD;
youth of the bars at low M, which is a consequence of downsizing. Young bars, being generally shorter and weaker, have not&#xD;
yet had time to form BPs. At high mass, while we find a plateau, the value is at ∼ 60 per cent whereas observations saturate at&#xD;
100 per cent. We attribute this difference to excessive heating in TNG50 due to merger activity and numerical resolution effects.&#xD;
BPs in TNG50 tend to occur in galaxies with more quiescent merger histories. As a result, the main driver of whether a bar hosts&#xD;
a BP in TNG50 is not the galaxy mass, but how long and strong the bar is. Separating the BP sample into those that have visibly&#xD;
buckled and those that have not, we find that fully half of BP galaxies show clear signs of buckling, despite the excessive heating&#xD;
and limited vertical resolution of TNG50.</description>
    <dc:date>2024-01-01T00:00:00Z</dc:date>
  </item>
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