<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-09-24T23:05:08Z</responseDate><request verb="GetRecord" identifier="oai:www.repository.cam.ac.uk:1810/277582" metadataPrefix="uketd_dc">https://api.repository.cam.ac.uk/server/oai/request</request><GetRecord><record><header><identifier>oai:www.repository.cam.ac.uk:1810/277582</identifier><datestamp>2019-01-31T15:59:12Z</datestamp><setSpec>com_1810_721</setSpec><setSpec>com_1810_256064</setSpec><setSpec>col_1810_218856</setSpec></header><metadata><uketd_dc:uketddc xmlns:uketd_dc="http://naca.central.cranfield.ac.uk/ethos-oai/2.0/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:uketdterms="http://naca.central.cranfield.ac.uk/ethos-oai/terms/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://naca.central.cranfield.ac.uk/ethos-oai/2.0/ http://naca.central.cranfield.ac.uk/ethos-oai/2.0/uketd_dc.xsd">
   <dc:title>Higher Order Structure in the Energy Landscapes of Model Glass Formers</dc:title>
   <dc:identifier xsi:type="dcterms:DOI">10.17863/CAM.24900</dc:identifier>
   <dc:creator>Niblett, Samuel Peter</dc:creator>
   <uketdterms:authoridentifier xsi:type="uketdterms:ORCID">0000000303370464</uketdterms:authoridentifier>
   <uketdterms:advisor>Wales, David</uketdterms:advisor>
   <uketdterms:authoridentifier xsi:type="uketdterms:ORCID">0000000235556645</uketdterms:authoridentifier>
   <dcterms:abstract>The study of supercooled liquids and glasses remains one of the most divisive and&#xd;
divided fields in modern physics. Despite a vast amount of effort and research time&#xd;
invested in this topic, the answers to many central questions remain disputed and&#xd;
incomplete. However, the link between the behaviour of supercooled liquids and&#xd;
their energy landscapes is well established and widely accepted. Understanding this&#xd;
link would be a key step towards resolving many of the mysteries and controversies&#xd;
surrounding the glass transition. Therefore the study of glassy energy landscapes is&#xd;
an important area of research.&#xd;
In this thesis, I report some of the most detailed computational studies of glassy&#xd;
potential energy landscapes ever performed. Using geometry optimisation techniques,&#xd;
I have sampled the local minima and saddle points of the landscapes for&#xd;
several supercooled liquids to analyse their dynamics and thermodynamics.&#xd;
Some of my analysis follows previous work on the binary Lennard-Jones fluid&#xd;
(BLJ), a model atomic liquid. BLJ is a fragile glass former, meaning that its&#xd;
transport coefficients have super-Arrhenius temperature dependence, rather than&#xd;
the more usual Arrhenius behaviour exhibited by strong liquids. The difference&#xd;
in behaviour between these two classes of liquid has previously been attributed to&#xd;
differing degrees of structure in the relevant energy landscapes.&#xd;
I have studied models for both fragile and strong glass formers: the molecular&#xd;
liquid ortho-terphenyl (OTP) and viscous silica (SiO$_{2}$) respectively. My results for&#xd;
OTP agree closely with trends observed for BLJ, suggesting that the same diffusion&#xd;
mechanism is applicable to fragile molecular liquids as well as to atomic. However,&#xd;
the dynamics and energy landscape of OTP are made complicated by the molecular&#xd;
orientational degrees of freedom, making the analysis more challenging for this&#xd;
system.&#xd;
Dynamics of BLJ, OTP and silica are all dominated by cage-breaking events:&#xd;
structural rearrangements in which atoms change their nearest neighbours. I propose&#xd;
a robust and general method to identify cage breaks for small rigid molecules, and&#xd;
compare some properties of cage breaks between strong and fragile systems.&#xd;
The energy landscapes of BLJ and OTP both display hierarchical ordering of potential energy minima into metabasins. These metabasins can be detected by&#xd;
the cage-breaking method. It has previously been suggested that metabasins are&#xd;
responsible for super-Arrhenius behaviour, and are absent from the landscapes of&#xd;
strong liquids such as SiO2. My results indicate that metabasins are present on the&#xd;
silica landscape, but that they each contain fewer minima than metabasins in BLJ&#xd;
or OTP.&#xd;
Metabasins are associated with anticorrelated particle motion, mediated by reversed&#xd;
transitions between minima of the potential energy landscape. I show that&#xd;
accounting for time-correlation of particle displacement vectors is essential to describe&#xd;
super-Arrhenius behaviour in BLJ and OTP, but also required to reproduce&#xd;
strong behaviour in silica. I hypothesise that the difference between strong and fragile&#xd;
liquids arises from a longer correlation timescale in the latter case, and I suggest&#xd;
a number of ways in which this proposition could be tested.&#xd;
I have investigated the effect on the landscape of freezing the positions of some&#xd;
particles in a BLJ fluid. This “pinning” procedure induces a dynamical crossover&#xd;
that has been described as an equilibrium “pinning transition”, related to the hypothetical&#xd;
ideal glass transition. I show that the pinning transition is related to (and&#xd;
probably caused by) a dramatic change in the potential energy landscape.&#xd;
Pinning a large fraction of the particles in a supercooled liquid causes its energy&#xd;
landscape to acquire global structure and hence structure-seeking behaviour, very&#xd;
different from the landscape of a typical supercooled liquid. I provide a detailed&#xd;
description of this change in structure, and investigate the mechanism underlying&#xd;
it.&#xd;
I introduce a new algorithm for identifying hierarchical organisation of a landsape,&#xd;
which uses concepts related to the pinning transition but is applicable to&#xd;
unpinned liquids as well. This definition is complementary to metabasins, but the&#xd;
two methods often identify the same higher-order structures. The new “packings”&#xd;
algorithm offers a route to test thermodynamic theories of the glass transition in&#xd;
the context of the potential energy landscape.&#xd;
Over the course of this thesis, I discuss several different terms and methods to&#xd;
identify higher-order structures in the landscapes of model glass formers, and investigate&#xd;
how this organisation varies between different systems. Although little&#xd;
variation is immediately apparent between most glassy landscapes, deeper analysis&#xd;
reveals a surprising diversity, which has important implications for dynamical&#xd;
behaviour in the vicinity of the glass transition.</dcterms:abstract>
   <uketdterms:institution>University of Cambridge</uketdterms:institution>
   <dcterms:issued>2018-07-20</dcterms:issued>
   <dc:type>Thesis</dc:type>
   <uketdterms:qualificationlevel>Doctoral</uketdterms:qualificationlevel>
   <uketdterms:qualificationname>Doctor of Philosophy (PhD)</uketdterms:qualificationname>
   <dc:language>en</dc:language>
   <uketdterms:sponsor>PhD studentship funded by the Cambridge Home Student Scholarship scheme and the Department of Chemistry</uketdterms:sponsor>
   <dcterms:isReferencedBy xsi:type="dcterms:URI">https://www.repository.cam.ac.uk/handle/1810/277582</dcterms:isReferencedBy>
   <dc:identifier xsi:type="dcterms:URI">https://apollo8-f-pro.lib.cam.ac.uk/bitstreams/8f43f3d0-4c61-4121-8a74-178b0d86c853/download</dc:identifier>
   <uketdterms:checksum xsi:type="uketdterms:MD5">23df301a6a2613328465143318129670</uketdterms:checksum>
   <dcterms:license>https://apollo8-f-pro.lib.cam.ac.uk/bitstreams/a0def0e0-99a2-4975-b692-596e1cb407a1/download</dcterms:license>
   <uketdterms:checksum xsi:type="uketdterms:MD5">87eda9de84448d1f82354d60eee3eb5f</uketdterms:checksum>
   <dc:rights>https://creativecommons.org/licenses/by-nc-sa/4.0/</dc:rights>
   <dc:subject>Potential Energy Landscape</dc:subject>
   <dc:subject>Glass Transition</dc:subject>
   <dc:subject>Supercooled Liquid</dc:subject>
   <dc:subject>Theoretical Chemistry</dc:subject>
   <dc:subject>Statistical Physics</dc:subject>
   <dc:subject>Fragility</dc:subject>
   <dc:subject>Random Pinning</dc:subject>
</uketd_dc:uketddc>
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