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    <title>FIHM Groups</title>
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    <description>Recent content on FIHM Groups</description>
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    <item>
      <title>Matt Cliffe</title>
      <link>//fihm.co.uk/people/mattcliffe/</link>
      <pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/people/mattcliffe/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/people/MattCliffe.jpg&#34; alt=&#34;Matt Cliffe&#34; title=&#34;Matt Cliffe&#34;&gt;&lt;/p&gt;&#xA;&lt;h4 id=&#34;mjc222atcamacuk&#34;&gt;mjc222[at]cam.ac.uk&lt;/h4&gt;&#xA;&lt;p&gt;Matt is an Associate Professor at the University of Cambridge in the Department of Materials Science and Metallurgy and leader of the FIHM group.&lt;/p&gt;&#xA;&lt;p&gt;Previously he was an Associate Professor at the University of Nottingham in the School of Chemistry and was a Research Fellowship at Sidney Sussex College at the University of Cambridge, where he worked with &lt;a href=&#34;http://www.ch.cam.ac.uk/group/grey/index&#34;&gt;Prof. Clare Grey&lt;/a&gt;. Matt gained his DPhil at the University of Oxford under the supervision of &lt;a href=&#34;https://goodwingroupox.uk/&#34;&gt;Prof. Andrew Goodwin&lt;/a&gt; on the characterization of disordered framework materials.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Rinku Kushwaha</title>
      <link>//fihm.co.uk/people/rinkukushwaha/</link>
      <pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/people/rinkukushwaha/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/people/RinkuKushwaha.jpg&#34; alt=&#34;Rinku Kushwaha&#34; title=&#34;Rinku Kushwaha&#34;&gt;&lt;/p&gt;&#xA;&lt;h4 id=&#34;rk825atcamacuk&#34;&gt;rk825[at]cam.ac.uk&lt;/h4&gt;&#xA;&lt;p&gt;Rinku joined the Functional Inorganic and Hybrid Materials group as a Postdoctoral Research Associate (PDRA). His research explores the magnetic and conducting properties resulting from doping in metal–organic frameworks (MOF). He comes from Uttar Pradesh, India. Rinku obtained his bachelor&amp;rsquo;s degree from the University of Allahabad and later joined the Indian Institute of Science Education and Research (IISER), Pune, for an integrated MS-PhD program. He completed his Ph.D. in Chemistry under the supervision of Prof. R. Vaidhyanathan (FRSC) on &amp;lsquo;Redox-active 2D Covalent Organic Frameworks for Energy Storage and Proton Conduction&amp;rsquo;. Outside his academic pursuits, he loves watching cricket and enjoys playing chess in his free time.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Luis León Alcaide</title>
      <link>//fihm.co.uk/people/luisleonalcaide/</link>
      <pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/people/luisleonalcaide/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/people/LuisLeonAlcaide.jpg&#34; alt=&#34;Luis León Alcaide&#34; title=&#34;Luis León Alcaide&#34;&gt;&lt;/p&gt;&#xA;&lt;h4 id=&#34;ll824atcamacuk&#34;&gt;ll824[at]cam.ac.uk&lt;/h4&gt;&#xA;&lt;p&gt;Luis León joined the FIHM Group as a Postdoctoral Research Associate, where he investigates highly frustrated MOF networks to explore novel magnetic behaviors. He completed his PhD in Nanoscience and Nanotechnology in 2024 at ICMOL, University of Valencia, Spain, under the supervision of Professor Mínguez Espallargas. Outside of his academic work, Luis enjoys food—especially when paired with a good wine—and is an avid basketball fan.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Takuya Ohmi, 大見 拓也</title>
      <link>//fihm.co.uk/people/takuyaohmi/</link>
      <pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/people/takuyaohmi/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/people/TakuyaOhmi.jpg&#34; alt=&#34;Takuya Ohmi, 大見 拓也&#34; title=&#34;Takuya Ohmi&#34;&gt;&lt;/p&gt;&#xA;&lt;h4 id=&#34;to377atcamacuk&#34;&gt;to377[at]cam.ac.uk&lt;/h4&gt;&#xA;&lt;p&gt;Takuya is a Postdoctoral Research Fellow of the Japan Society for the Promotion of Science (JSPS) in the FIHM Group. He received his PhD from the Institute of Science Tokyo on crystal structure control in defect-ordered organic-inorganic hybrid perovskites. His research focuses on the synthesis and characterisation of new functional materials, particularly organic-inorganic hybrid compounds. Outside of research, he enjoys running and travelling.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Xiaoxuan Su , 苏晓轩</title>
      <link>//fihm.co.uk/people/xiaoxuansu/</link>
      <pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/people/xiaoxuansu/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/people/XiaoxuanSu.png&#34; alt=&#34;Xiaoxuan Su, 苏晓轩&#34; title=&#34;Xiaoxuan Su, 苏晓轩&#34;&gt;&lt;/p&gt;&#xA;&lt;h4 id=&#34;xs346atcamacuk&#34;&gt;xs346[at]cam.ac.uk&lt;/h4&gt;&#xA;&lt;p&gt;Xiaoxuan earned his Master&amp;rsquo;s degree in Chemistry from the University of Sheffield in 2021, returned to China and worked as a research assistant for two years before deciding to pursue his Ph.D joint between the Pilgrim and FIHM Groups. During his spare time, he enjoys reading and playing board games.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Amos Blyth</title>
      <link>//fihm.co.uk/people/amosblyth/</link>
      <pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/people/amosblyth/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/people/AmosBlyth.jpg&#34; alt=&#34;Amos Blyth&#34; title=&#34;Amos Blyth&#34;&gt;&lt;/p&gt;&#xA;&lt;h4 id=&#34;aeb204atcamacuk&#34;&gt;aeb204[at]cam.ac.uk&lt;/h4&gt;&#xA;&lt;p&gt;Amos completed his master’s research with the FIHM group in 2023 and returned in 2024 to undertake a PhD in quantum radical metal organic frameworks. His work focuses on investigating the local structure of two- and three-dimensional frameworks using X-ray and electron pair distribution function (PDF) analysis.&lt;/p&gt;&#xA;&lt;p&gt;Amos loves to bird watch and sends much of his free time doing this. Else, he’ll be out running, sitting with a coffee in his rocking chair reading or crocheting, or playing video games.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Kuba Lemanski</title>
      <link>//fihm.co.uk/people/kubalemanski/</link>
      <pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/people/kubalemanski/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/people/KubaLemanski.png&#34; alt=&#34;Kuba Lemanski&#34; title=&#34;Kuba Lemanski&#34;&gt;&lt;/p&gt;&#xA;&lt;h4 id=&#34;kubalemanskiatnottinghamacuk&#34;&gt;Kuba.Lemanski[at]nottingham.ac.uk&lt;/h4&gt;&#xA;&lt;p&gt;Kuba is a PhD student working on the DISCO-MOF project with a background in inorganic chemistry. His research focuses on the preparation of radical ligand MOFs with early transition metals and investigating their properties.&#xA;Outside of chemistry he loves spending time in nature, hiking, cycling and especially running. Some of his other interests include cooking, travelling and gaming as well as trying as many types of tea as possible (current favourite being apple strudel).&lt;/p&gt;</description>
    </item>
    <item>
      <title>Mason Ormsby</title>
      <link>//fihm.co.uk/people/masonormsby/</link>
      <pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/people/masonormsby/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/people/masonormsby.jpg&#34; alt=&#34;Mason Ormsby&#34; title=&#34;Mason Ormsby&#34;&gt;&lt;/p&gt;&#xA;&lt;h4 id=&#34;masonormsbyatnottinghamacuk&#34;&gt;Mason.Ormsby[at]nottingham.ac.uk&lt;/h4&gt;&#xA;&lt;p&gt;Mason completed his undergraduate studies with First Class Honours in Chemistry from Nottingham Trent University in 2024. Taking a year out to work as an account executive, he decided to pursue a masters, working within the Pilgrim group and FIHM group. In his spare time, he enjoys playing games and going to the gym.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Alumni</title>
      <link>//fihm.co.uk/people/alumni/</link>
      <pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/people/alumni/</guid>
      <description>&lt;ul&gt;&#xA;&lt;li&gt;&#xA;&lt;p&gt;2024-25, Joseph Ogar (PDRA), &lt;a href=&#34;https://www.ntu.ac.uk/staff-profiles/science-technology/joseph-ogar&#34;&gt;Senior Lecturer, Nottingham Trent University&lt;/a&gt;&lt;/p&gt;&#xA;&lt;/li&gt;&#xA;&lt;li&gt;&#xA;&lt;p&gt;2022-25, Simrun Lata (PhD), &lt;a href=&#34;https://www.thenamilab.com/&#34;&gt;PhD, NAMI Group, University of Nottingham&lt;/a&gt;&lt;/p&gt;&#xA;&lt;/li&gt;&#xA;&lt;li&gt;&#xA;&lt;p&gt;2020-24, Andrew Jones (PhD), &lt;a href=&#34;https://uchybridmaterials.com/&#34;&gt;PDRA, Bennett Group, University of Canterbury&lt;/a&gt;&lt;/p&gt;&#xA;&lt;/li&gt;&#xA;&lt;li&gt;&#xA;&lt;p&gt;2020-23, 2018-19 Madeleine Geers (PhD, MSci), &lt;a href=&#34;https://www.uu.se/en/contact-and-organisation/staff?query=N20-324&#34;&gt;PDRA, Clulow Group, Uppsala University&lt;/a&gt;&lt;/p&gt;&#xA;&lt;/li&gt;&#xA;&lt;li&gt;&#xA;&lt;p&gt;2019-23 Jem Pitcairn (PhD, PDRA), &lt;a href=&#34;https://clarkgroupbirmingham.com/&#34;&gt;PDRA, Clark Group, University of Birmingham&lt;/a&gt;&lt;/p&gt;&#xA;&lt;/li&gt;&#xA;&lt;li&gt;&#xA;&lt;p&gt;2021-23 Olukayode Babarinde (PhD) &lt;a href=&#34;https://www.funeralguide.co.uk/obituaries/128369&#34;&gt;Nigerian Defence Academy, sadly deceased&lt;/a&gt;&lt;/p&gt;&#xA;&lt;/li&gt;&#xA;&lt;li&gt;&#xA;&lt;p&gt;2020-21 Claire Housely (PhD), &lt;a href=&#34;https://commonslibrary.parliament.uk/authors/claire-housley/&#34;&gt;Senior Nuclear Policy Advisor, Dept. for Energy Security and Net Zero&lt;/a&gt;, &lt;a href=&#34;https:/twitter.com/stringatheory&#34;&gt;@StringaTheory&lt;/a&gt;&lt;/p&gt;&#xA;&lt;/li&gt;&#xA;&lt;li&gt;&#xA;&lt;p&gt;2016-21 Francesca Firth (MSci, PhD), &lt;a href=&#34;https://veranova.com/&#34;&gt;Veranova&lt;/a&gt;, &lt;a href=&#34;https://twitter.com/FC_Firth&#34;&gt;@FC_Firth&lt;/a&gt;&lt;/p&gt;</description>
    </item>
    <item>
      <title>A glass full of magnetism</title>
      <link>//fihm.co.uk/publications/nc_2025_femofglass/</link>
      <pubDate>Tue, 07 Apr 2026 08:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/nc_2025_femofglass/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/nc_2025_FeMOFGlass.png&#34; alt=&#34;Fig. 1 Picture of a MOF glass sample and schematic of the atomic scale disordered structure&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;Glasses are familiar materials, yet their atomic-scale organisation and physical properties remain difficult to fully understand. This challenge is particularly pronounced for magnetic glasses, where structural disorder strongly affects collective spin behaviour. Most conventional glasses are chemically simple inorganic systems, which limits their tunability and functionality. Metal–organic frameworks (MOFs) combine metal ions and organic linkers, and so by using organic chemistry to create different organic linker molecules, we have the ability to control the magnetic behaviour of MOFs.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Remixing 2D magnets</title>
      <link>//fihm.co.uk/publications/cc_2024_tune_vdw_mom/</link>
      <pubDate>Sun, 17 Nov 2024 18:50:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/cc_2024_tune_vdw_mom/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/cc_2024_tuning.png&#34; alt=&#34;Tuning the properties of a layered magnet&#34; title=&#34;Swapping S for O makes this a softer magnet, but a harder material.&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;One of the key attractions of metal-organic materials is their variety: organic molecules can be tweaked and refashioned almost indefinitely. We have recently reported a new &lt;a href=&#34;//fihm.co.uk/publications/jacs_2024_nifecl2l/&#34;&gt;&amp;lsquo;crinkly magnet&amp;rsquo;&lt;/a&gt;, nickel dichloride 2,1,3-benzothiadizole (btd), with an unusual &amp;ldquo;noncollinear&amp;rdquo; magnetic structure. In this paper we explore what happens when the sulfur atom in btd is swapped for an oxygen atom.&lt;/p&gt;</description>
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    <item>
      <title>Surfing the (mag)net</title>
      <link>//fihm.co.uk/publications/acscs_2024_magnet/</link>
      <pubDate>Thu, 12 Sep 2024 08:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/acscs_2024_magnet/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/acs_2024_MagNet.png&#34; alt=&#34;Magnetic diffuse scattering (background) and nets (foreground)&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;A net is a periodic (repeating) series of connected points. This concept is at the heart of solid state science because we often think of the chemical structures of materials as comprising atoms connected by bonds, which therefore form a net. The underlying net of a material allows for classification&amp;mdash;is this structure related to that structure&amp;mdash;but also prediction of its properties, e.g. is it likely to be stiff or soft. Although there are an infinite number of possible nets, the best estimate is that there are only twenty nets with only one kind of vertex and edge.&lt;sup id=&#34;fnref:1&#34;&gt;&lt;a href=&#34;#fn:1&#34; class=&#34;footnote-ref&#34; role=&#34;doc-noteref&#34;&gt;1&lt;/a&gt;&lt;/sup&gt; Most of these will be familiar, at least to chemists, like the simple cubic &lt;strong&gt;pcu&lt;/strong&gt; net beloved of scaffolders or the face-centred cubic &lt;strong&gt;fcu&lt;/strong&gt; net that emerges in pyramidal stacks of oranges. There&amp;rsquo;s a particular interest in the nets which are not bipartite (i.e. the points of the net can&amp;rsquo;t be coloured in red and blue such that no red neighbours another red and no blue a blue, normally containing a triangle), because these can very have unusual magnetic properties. In these non-bipartite nets, if a magnetic spin is put at every node and they interact such that the spins prefer to point in opposite directions, that is, they are antiferromagnetically coupled, there are very many states there are nearly equal in energy: they are &lt;em&gt;frustrated&lt;/em&gt;.&lt;/p&gt;</description>
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    <item>
      <title>All iNCSlusive</title>
      <link>//fihm.co.uk/publications/ic_2024_thiocyanates/</link>
      <pubDate>Tue, 09 Jul 2024 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/ic_2024_thiocyanates/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/IC_periodic_thiocyanate.png&#34; alt=&#34;Periodic table of thiocyanate&#34; title=&#34;Periodic table of thiocyanate&#34;&gt;&#xA;&lt;em&gt;Figure: Periodic table of thiocyanates, showing the state of our knowledge&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;There are 118 elements and we are now confident that there will be no more stable elements discovered. Equally, we&amp;rsquo;re fairly confident that there won&amp;rsquo;t be many (if any) binary compounds made with stable elements. You might assume that this settled state of knowledge is correct for other simple compounds; however, this isn&amp;rsquo;t true.&lt;/p&gt;</description>
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      <title>Crinkle cut magnets </title>
      <link>//fihm.co.uk/publications/jacs_2024_nifecl2l/</link>
      <pubDate>Tue, 02 Jul 2024 10:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/jacs_2024_nifecl2l/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/jacs_2024_cant_patrol.gif&#34; alt=&#34;MCl2L&#34; title=&#34;Figure 1.&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;em&gt;Figure 1. A schematic illustration of how tilting ferromagnetic chains with strong single ion anisotropy can produce a noncollinear structure with a net moment&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;In most magnetic materials, the underlying atomic spins line up either parallel (ferromagnetic correlation) or antiparallel (antiferromagnetic correlation): they are collinear. In noncollinear magnets spins can arrange themselves in any direction relative to each other (depending on the interactions and geometry of the material) and these noncollinear spin textures can produce magnetic properties that are hard to realise otherwise, including electrical control over magnetic spin or nanometric magnetic data storage. Creating materials with these noncollinear structures is challenging, however, because they typically require multiple different spin-spin interactions to be competitive with each other.&lt;/p&gt;</description>
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      <title>A molecular framework honeycomb magnet</title>
      <link>//fihm.co.uk/publications/pccp_2024_namnncs3_honeycomb/</link>
      <pubDate>Mon, 20 May 2024 10:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/pccp_2024_namnncs3_honeycomb/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/NaMnNCS3_honeycomb.png&#34; alt=&#34;[Na(OH2)3]Mn(NCS)3&#34; title=&#34;[Na(OH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;]Mn(NCS)&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; has a perfect honeycomb structure and so is a good experimental realisation of the magnetic honeycomb.&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;In this paper we investigate a metal thiocyanate compound [Na(OH&lt;sub&gt;2&lt;/sub&gt;)&lt;sub&gt;3&lt;/sub&gt;]Mn(NCS)&lt;sub&gt;3&lt;/sub&gt; which consists of rods of a honeycomb manganese thiocyanate network threaded by rods consisting of sodium cations and water. This structure has perfect three-fold symmetry, but unusually, the manganese atom do not lie on an inversion centre (i.e. each metal atom knows which way up it is), although the crystal as a whole does have inversion symmetry.&lt;/p&gt;</description>
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      <title>High pressure behaviour of the magnetic van der Waals molecular framework Ni(NCS)&lt;sub&gt;2&lt;/sub&gt;</title>
      <link>//fihm.co.uk/publications/prb_2023_nincs2/</link>
      <pubDate>Tue, 31 Oct 2023 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/prb_2023_nincs2/</guid>
      <description>&lt;p&gt;&lt;strong&gt;Summary by Madeleine Geers&lt;/strong&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;em&gt;Selected as &lt;a href=&#34;https://journals.aps.org/prb/highlights&#34;&gt;Editor&amp;rsquo;s Suggestion&lt;/a&gt;&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/PRB_NiSCN2_elephant.png&#34; alt=&#34;Ni(NCS)2&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;em&gt;We investigated what would happen to Ni(NCS)&lt;sub&gt;2&lt;/sub&gt; when subjected to the force of an elephant over a square centimetre. Elephant by &lt;a href=&#34;https://pixabay.com/users/creozavr-2567670/?utm_source=link-attribution&amp;amp;utm_medium=referral&amp;amp;utm_campaign=image&amp;amp;utm_content=3526681.&#34;&gt;Dmitry Abramov&lt;/a&gt;&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;Detecting pressure changes plays an essential role in our everyday lives, from biomedical applications such as assessing adhesion of prosthetics, to entering a code on a PIN pad or monitoring gas flow on planes. Often we cannot measure pressure changes directly, so identifying materials whose physical properties, such as magnetism, change when a pressure is applied can be very useful. Two-dimensional, or &amp;ldquo;van der Waals&amp;rdquo;, materials are particularly exciting for this kind of application. The atoms in 2D materials are strongly bonded in two directions, whilst having weak &amp;ldquo;dispersion&amp;rdquo; or van der Waals forces along the third axis: with graphite being the most famous example. If a material is magnetic, the temperature at which it magnetically orders can be increased quite a lot by applying pressure, for example the 2D magnetic material NiI&lt;sub&gt;2&lt;/sub&gt; increases its magnetic ordering temperature by 235 K when compressed to 190 kbar, an increase of +1.6 % kbar&lt;sup&gt;–1&lt;/sup&gt;. 190 kbar is a considerable pressure:  James Cameron in his submarine reached pressures of 1 kbar at the bottom of the Mariana trench and a typical volcano erupts with between 0.2–3 kbar of pressure. It would be useful to have materials which show big changes at more everyday pressures.&lt;/p&gt;</description>
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    <item>
      <title>An open source webtool for calculating compressibilities &amp; thermal expansion</title>
      <link>//fihm.co.uk/publications/joss_2023_pascal/</link>
      <pubDate>Sun, 22 Oct 2023 18:44:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/joss_2023_pascal/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/JOSS_2023_PASCal.png&#34; alt=&#34;PASCal&#34; title=&#34;PASCal Logo&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;em&gt;Figure: PASCal Logo shows an indicatrix, which plots the anisotropy of response of a crystal.&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;This paper describes the newest version of &lt;a href=&#34;http://www.pascalapp.co.uk&#34;&gt;PASCal&lt;/a&gt;, a simple webtool designed to calculate the principal thermal expansivities, compressibilities or response to electrochemical strain of a system from lattice parameters. For low symmetry crystals, the arbitrary choice of unit cell means that if you only look at the cell lengths, it is possible to miss interesting features in the (thermo)mechanical behaviour of a crystal, for example negative thermal expansion or negative compressibilities.&#xA;PASCal is designed to be an easy method for calculating the principal strain values that give the complete description of these systems.&#xA;The new version is completely open source, available offline and includes electrochemical strain.&lt;/p&gt;</description>
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    <item>
      <title></title>
      <link>//fihm.co.uk/programs/pascal-v2/</link>
      <pubDate>Fri, 10 Mar 2023 12:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/programs/pascal-v2/</guid>
      <description></description>
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      <title>Nature inspired complex magnetic order</title>
      <link>//fihm.co.uk/publications/cs_2023_csmncs3/</link>
      <pubDate>Fri, 10 Mar 2023 12:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/cs_2023_csmncs3/</guid>
      <description>&lt;p&gt;&lt;strong&gt;Summary by Maddie Geers&lt;/strong&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/cs_CsMNCS3_magnet.png&#34; alt=&#34;Fig. 1 Complex magnetic order emerges in post-perovskite metals thiocyanates.&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;Nature is a deep-rooted source of inspiration for innovations, a notion continually woven into our everyday lives. Magnesium silicate (MgSiO&lt;sub&gt;3&lt;/sub&gt;) is one of the most abundant minerals on Earth and about 20 years ago it was discovered to undergo a structural transition. In most of the Earth&amp;rsquo;s mantle, magnesium silicate adopts the perovskite structure, however, plunging to the lower depths of the Earth’s mantle it evolves to have the post-perovskite structure. The high temperatures and pressures needed for this transition to occur (1200 K and 120 GPa) make studying this compound very challenging, so identifying compounds that exhibit the post-perovskite structure at atmospheric pressure is a useful task. One method to achieve this is by replacing the atomic oxygen anions with molecular anions, for example dicyanimide (NCNCN&lt;sup&gt;–&lt;/sup&gt;) or thiocyanate (NCS&lt;sup&gt;–&lt;/sup&gt;) ligands.&lt;/p&gt;</description>
    </item>
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      <title>Designing quantum phases in metal-organic magnets</title>
      <link>//fihm.co.uk/publications/jacs_2023_crpymcl2/</link>
      <pubDate>Mon, 09 Jan 2023 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/jacs_2023_crpymcl2/</guid>
      <description>&lt;p&gt;&lt;strong&gt;Summary by Jem Pitcairn&lt;/strong&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/jacs_2023_CrPymCl2.png&#34; alt=&#34;Cr(Pym)Cl2&#34; title=&#34;Figure 1. Left: the structure of CrCl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(Pym), showing the alternating spin chains weakly coupled by the organic molecules. Right: Inelastic neutron scattering (INS) measurements and calculations which allowed us to measure the strength of the magnetic interactions.&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;em&gt;Figure 1. Left: the structure of CrCl&lt;sub&gt;2&lt;/sub&gt;(Pym), showing the alternating spin chains weakly coupled by the organic molecules. Right: Inelastic neutron scattering (INS) measurements and calculations which allowed us to measure the strength of the magnetic interactions.&lt;/em&gt;&lt;/p&gt;</description>
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      <title>At the end of the tether</title>
      <link>//fihm.co.uk/publications/ic_2022_tether/</link>
      <pubDate>Sat, 31 Dec 2022 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/ic_2022_tether/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/ic_2022_tether.jpeg&#34; alt=&#34;Tethering Figure&#34; title=&#34;Schematic diagram of the behaviour of oligoMOFs&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;em&gt;Figure 1: Schematic diagram of the behaviour of oligoMOFs&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;A summary of this paper can be found in &lt;a href=&#34;https://www.nature.com/articles/s41570-022-00426-1&#34;&gt;Nature Reviews Chemistry&lt;/a&gt;.&lt;/p&gt;&#xA;&lt;p&gt;This work was led by Prof Seth Cohen at the University of California, San Diego.&lt;/p&gt;</description>
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      <title>Long-distance (magnetic) relationship</title>
      <link>//fihm.co.uk/publications/cec_2022_crbiscn6_mag/</link>
      <pubDate>Sun, 26 Jun 2022 12:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/cec_2022_crbiscn6_mag/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/cec_CrBiSCN6.png&#34; alt=&#34;Fig. 1 Magnetic order in CrBi(SCN)6.&#34;&gt;&#xA;&lt;em&gt;Figure. 1&lt;/em&gt; Magnetic order in CrBi(SCN)&lt;sub&gt;6&lt;/sub&gt;. Left: the magnetic superexchange pathways. Right: Neutron diffraction data showing magnetic order.&lt;/p&gt;&#xA;&lt;p&gt;Ions with unpaired electrons are magnetic and when those magnetic ions are assembled into a crystalline solid, their magnetic spins interact. At low enough temperatures, these spins therefore typically lock into an ordered state. The temperature at which this ordering happens depends, however, on the strength of the magnetic &amp;rsquo;exchange&amp;rsquo; interactions between the spins, which is strong for ions next to each other (&lt;em&gt;e.g.&lt;/em&gt; in magnetite, Fe&lt;sub&gt;3&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt;) but gets rapidly weaker as the magnetic ions are separated by more intervening atoms (&lt;em&gt;e.g.&lt;/em&gt; chrome alum, KCr(SO&lt;sub&gt;4&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;.12H&lt;sub&gt;2&lt;/sub&gt;O). In crystals where the magnetic ions are connected by multiple multi-atomic molecules this means that the temperature at which magnetic ordering occurs can very often be too cold to practically measure (as low as 0.05K, i.e. within a twentieth of a degree of absolute zero).&lt;/p&gt;</description>
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      <title>Tracking the formation of MOFs in solution</title>
      <link>//fihm.co.uk/publications/jacs_2021_insitu_pdf_uio/</link>
      <pubDate>Wed, 17 Nov 2021 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/jacs_2021_insitu_pdf_uio/</guid>
      <description>&lt;p&gt;&lt;strong&gt;Summary by Francesca Firth&lt;/strong&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/jacs_2021_insitu_UiO.png&#34; alt=&#34;Schematic of MOF formation&#34; title=&#34;Figure 1: Schematic of MOF formation&#34;&gt;&#xA;&lt;em&gt;Figure 1: Schematic of stages in the formation of hcp UiO-66(Hf) in solvothermal conditions, through different cluster intermediates.&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;Metal-organic frameworks (MOFs) are of great interest for applications such as energy storage and carbon capture, particularly due to their outstanding chemical tunability. In particular, zirconium (Zr) and hafnium (Hf) MOFs are promising for real-world applications because they are very stable. Our previous work discovered that changing the synthesis conditions, including which solvent was used what temperature the reaction was carried out, changed the structure of the MOF that formed for the important UiO family of MOFs. In particular we found that we could &lt;a href=&#34;//fihm.co.uk/publications/nc_2014_mof_defects&#34;&gt;introduce missing clusters&lt;/a&gt; or make MOFs with &amp;lsquo;double&amp;rsquo; Hf&lt;sub&gt;12&lt;/sub&gt; &lt;a href=&#34;//fihm.co.uk/publications/jacs_2017_uio-67_nanosheets&#34;&gt;clusters&lt;/a&gt;, rather than classic UiO Hf&lt;sub&gt;6&lt;/sub&gt; clusters. These new MOF structures have very different chemical and physical properties.&lt;/p&gt;</description>
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      <title>Combining complex orders in perovskites</title>
      <link>//fihm.co.uk/publications/cs_2020_anibiscn6/</link>
      <pubDate>Fri, 04 Dec 2020 12:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/cs_2020_anibiscn6/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/ANiBiSCN6_intro.png&#34; alt=&#34;Fig. 1 Combining multiple orderings is possible in A{NiBi(SCN)$_6$} perovskites through the A site cations.&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;Many of the most useful properties of materials arise from the collective ordering of many individual nanoscale components across an entire crystal: for example, ferromagnetism is the result of aligning the magnetic spins within a material and ferroelectricity is the ordering of polar electric distortions. One way to create new properties in materials is therefore to order simultaneously multiple different features at once (&lt;em&gt;e.g.&lt;/em&gt; combining ferromagnetic order with ferroelectric order to create magnetic and electric &amp;lsquo;multiferroics&amp;rsquo;). Making use of this strategy, however, means confronting the general tendency for materials towards disorder.&lt;/p&gt;</description>
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      <title>Layered magnetic molecular-frameworks</title>
      <link>//fihm.co.uk/publications/ic_2020_mncs2/</link>
      <pubDate>Mon, 20 Jul 2020 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/ic_2020_mncs2/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/IC_MNCS2.png&#34; alt=&#34;Structure and magnetism of M(NCS)2&#34; title=&#34;divalent metal thiocyanate summary&#34;&gt;&#xA;&lt;em&gt;Figure: Structure and magnetic properties of the magnetic molecular frameworks M(NCS)&lt;sub&gt;2&lt;/sub&gt; (M = Mn, Fe, Co, Ni). Left: the chemical structure of the M(NCS)2 frameworks; centre: the net magnetic interaction strength for each framework and right: the magnetic structures of M(NCS)&lt;sub&gt;2&lt;/sub&gt;, with arrows denoting the relative orientation of the bar magnets. The magnetic structures of Mn(NCS)&lt;sub&gt;2&lt;/sub&gt;, Fe(NCS)&lt;sub&gt;2&lt;/sub&gt; and Co(NCS)&lt;sub&gt;2&lt;/sub&gt; are in orange, and in blue for Ni(NCS)&lt;sub&gt;2&lt;/sub&gt;.&lt;/em&gt;&lt;/p&gt;</description>
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      <title>Directly detecting defect domains</title>
      <link>//fihm.co.uk/publications/jacs_2020_uio-66_sed/</link>
      <pubDate>Fri, 17 Jul 2020 00:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/jacs_2020_uio-66_sed/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/jacs_2020_SED_UiO.png&#34; alt=&#34;Scanning electron diffraction images of defect domains&#34; title=&#34;Scanning electron diffraction images of defect domains&#34;&gt;&#xA;&lt;em&gt;Figure: Scanning electron diffraction images of UiO-66. Top: a single crystal of UiO-66 visualised in (purple). Bottom: the defect nanodomains (green).&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;Defects are key to the properties of all kinds of materials, from silicon chips to turbine blades. Metal-organic frameworks (MOFs) are no exception. Previously, &lt;a href=&#34;%7B%7B.Site.BaseURL%7D%7D/publications/nc_2014_mof_defects/&#34;&gt;we have shown&lt;/a&gt; that nanodomains consisting of a more open structure can be produced within crystals of the most important MOFs, so-called UiO-66, by controlling the synthesis. In this paper, we collaborated with teams based at the &lt;a href=&#34;https://www.emg.msm.cam.ac.uk/People/dnj23&#34;&gt;Universities of Cambridge&lt;/a&gt; and &lt;a href=&#34;https://eps.leeds.ac.uk/chemical-engineering/staff/8179/dr-sean-collins&#34;&gt;Leeds&lt;/a&gt; who are experts in an emerging technique, scanning electron diffraction (SED), which allowed us to image directly entire defect nanodomains in a MOF for the first time.&lt;/p&gt;</description>
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      <title>Diverse defects in metal thiocyanate frameworks</title>
      <link>//fihm.co.uk/publications/cs_2020_defect_ncs/</link>
      <pubDate>Fri, 07 Feb 2020 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/cs_2020_defect_ncs/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/defect_perovskite_small.png&#34; alt=&#34;Defects in thiocyanate Prussian Blues&#34; title=&#34;Range of defects in different thiocyanate frameworks&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;&amp;ldquo;Your imperfections are what make you perfect&amp;rdquo; is not just a twee word-art slogan on the wall of a chain coffee shop but also a guide for materials chemistry. Defects, the deviations from perfect crystalline order, are key to producing the useful properties of many solids, from solar cells to gemstones. The challenge facing chemists, however, is that defects are hard to see: there are not many of them and they are usually randomly distributed throughout the material. This means that standard crystallographic techniques, which rely on long-range order, are much less useful. As a result, it is very challenging to know what defects are present in a material, even if we can see their consequences.&lt;/p&gt;</description>
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      <title>SquidLab</title>
      <link>//fihm.co.uk/publications/revsciinst_squidlab/</link>
      <pubDate>Fri, 07 Feb 2020 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/revsciinst_squidlab/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/RevSciInst_SquidLabLogo_small.png&#34; alt=&#34;SquidLab Logo&#34; title=&#34;SquidLab Logo&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;A team at the Universities of Warwick, Nottingham and Cambridge have developed open-source software for analysing magnetic data and allowing more sensitive measurements&lt;/p&gt;&#xA;&lt;p&gt;&lt;strong&gt;&lt;a href=&#34;https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/supermag/whoswho/matthew_coak/&#34;&gt;Summary by Dr Matt Coak&lt;/a&gt;&lt;/strong&gt;&lt;/p&gt;&#xA;&lt;p&gt;Measurements of magnetic properties in the lab are commonplace and essential across a range of physics, chemistry, materials science and even biology. There are many cases however where the magnetic signal of the sample holder or environment swamps that of the material to measure. Our new software, SquidLab, provides a powerful and flexible toolbox to remove magnetic backgrounds to recover the sample&amp;rsquo;s signal and allow measurements that were previously impossible.&lt;/p&gt;</description>
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      <title>Ionic and Electronic Conduction in TiNb&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;7&lt;/sub&gt;</title>
      <link>//fihm.co.uk/publications/jacs_2019_tinb2o7/</link>
      <pubDate>Mon, 09 Dec 2019 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/jacs_2019_tinb2o7/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/jacs_2019_tinb2o7.gif&#34; alt=&#34;Summary of the behavioiur of TiNb2O7&#34; title=&#34;Summary of the behavioiur of TiNb2O7&#34;&gt;&#xA;&lt;em&gt;Figure: TiNb&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;7&lt;/sub&gt; is a battery anode material, which allows lithium ions to rapidly pass through it and is a good electrical conductor when lithium is inserted into its structure.&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;This work was carried out in collaboration with the groups of Prof Clare Grey and Dr Siân Dutton at the University of Cambridge, Dr Andrew Morris at the University of Birmingham and Prof Graham Henkelman at the University of Texas.&lt;/p&gt;</description>
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      <title>Short-range ordering in a battery electrode, the ‘cation-disordered’ rocksalt Li&lt;sub&gt;1.25&lt;/sub&gt;Nb&lt;sub&gt;0.25&lt;/sub&gt;Mn&lt;sub&gt;0.5&lt;/sub&gt;O&lt;sub&gt;2&lt;/sub&gt;</title>
      <link>//fihm.co.uk/publications/cc_2019_corr_disorder_linbmno/</link>
      <pubDate>Mon, 01 Jul 2019 10:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/cc_2019_corr_disorder_linbmno/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/cc_2019_LiNbMnO.png&#34; alt=&#34;Powder diffraction data, left, X-ray crystal structure, centre, and battery performance, right, the the more ordered and less ordered forms of LiNbMnO.&#34; title=&#34;Powder diffraction data, left, X-ray crystal structure, centre, and battery performance, right, the the more ordered and less ordered forms of LiNbMnO.&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;em&gt;Powder diffraction data, left, X-ray crystal structure, centre, and battery performance, right, the the more ordered and less ordered forms of LiNbMnO.&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;This work was carried out in collaboration with the groups of Prof Clare Grey and Dr Siân Dutton at the University of Cambridge.&lt;/p&gt;</description>
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      <title>Faulty Goods? the exciting consequences of introducing defects in MOF frameworks with water</title>
      <link>//fihm.co.uk/publications/jma_2019_water_hcp_uio/</link>
      <pubDate>Wed, 20 Feb 2019 09:30:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/jma_2019_water_hcp_uio/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/jma_2019_H2O_defect_UiO.png&#34; alt=&#34;Water&amp;rsquo;s role in PXRD&#34; title=&#34;Water is a critical factor for the formation of **hcp** UiO phases, as shown by the powder X-ray diffraction pattern.&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;strong&gt;&lt;a href=&#34;https://www.ch.cam.ac.uk/person/fcnf2&#34;&gt;Summary by Francesca Firth&lt;/a&gt;&lt;/strong&gt;&lt;/p&gt;&#xA;&lt;p&gt;Reading the abstracts from conferences on fields ranging from crystallography through energy storage to the many branches of materials chemistry, it is a challenge to avoid spotting one on the subject of metal-organic frameworks (MOFs). With their incredible tunability and versatility, arising from the wide range of metal nodes and organic linkers available from which to build a multi-dimensional porous network, MOFs are the source of great excitement in the search for materials for all kinds of applications. However, changing the identity of the metal or linker is not the only method of altering the properties of the framework – the formation of defects, such as missing linkers, missing nodes, or stacking faults, in a structure can also significantly change the properties of a material (often with less disastrous consequences than a misplaced screw in a build-at-home chair&amp;hellip;). UiO family MOFs are ideal for studying defects, as their strong metal-linker coordination and high connectivity allow them to incorporate linker and metal-cluster vacancies to a high degree.&lt;/p&gt;</description>
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      <title>Thiocyanate &#39;Prussian Blues&#39;</title>
      <link>//fihm.co.uk/publications/cs_2018_mbiscn6/</link>
      <pubDate>Mon, 29 Oct 2018 11:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/cs_2018_mbiscn6/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/ChemSci_2018_MBiSCN.png&#34; alt=&#34;Structure and optical properties of iron(III) hexathiocyanatobismuthate&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;em&gt;Left: the structure of Fe[Bi(SCN)&lt;sub&gt;6&lt;/sub&gt;] determined using single crystal X-ray diffraction. Right: the optical absorption spectrum of M[Bi(SCN)&lt;sub&gt;6&lt;/sub&gt;], showing which wavelengths of light each compound absorbs.&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;Prussian Blue is an iconic material. Discovered around 1706, ostensibly by adding iron sulfate to a concotion of boiled animal blood and potassium carbonate, it was the first modern purely synthetic pigment. It made blue paint that wouldn&amp;rsquo;t fade available to artists at a low cost and perhaps most famously dyed the uniforms of the Royal Prussian Army from the early 18th century through to the 20th. Since then Prussian Blue and related compounds have been found to be useful for all kinds of applications, including electrochromics (materials that change colour when a voltage is applied to them), batteries, and even as magnets. Prussian Blue is also one of the most simple examples of a coordination polymer:  a material where metal atoms are connected by multi-atom linkers into infinite chains or frameworks. In this case, iron atoms are connected by cyanide (CN&lt;sup&gt;–&lt;/sup&gt;) into a three dimensional cubic network, with the chemical formula (Fe&lt;sup&gt;3+&lt;/sup&gt;&lt;sub&gt;4&lt;/sub&gt;[Fe&lt;sup&gt;2+&lt;/sup&gt;(CN)&lt;sub&gt;6&lt;/sub&gt;]&lt;sub&gt;3&lt;/sub&gt;)· &lt;em&gt;x&lt;/em&gt; H&lt;sub&gt;2&lt;/sub&gt;O.&lt;/p&gt;</description>
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      <title>How to use ToposPro to work out a topology of a framework</title>
      <link>//fihm.co.uk/posts/how_to_topology/</link>
      <pubDate>Mon, 01 Oct 2018 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/posts/how_to_topology/</guid>
      <description>&lt;p&gt;Topology is a very important way of classifying the connectivity of framework materials but ToposPro, the standard software for topological analysis can be quite intimidating. I am no mathematical topologist or ToposPro expert, but here is a short guide for how to take a CIF and analyse the topology of its simplified net. Much more information is available from the ToposPro &lt;a href=&#34;http://topospro.com&#34;&gt;website&lt;/a&gt; and &lt;a href=&#34;http://topospro.com/faq/manuals/l&#34;&gt;manual&lt;/a&gt;. If you would rather one of the experts deteremines the topology of your structure for you, the ToposPro team will now do this &lt;a href=&#34;https://topospro.com/online-tools/determining/&#34;&gt;for you&lt;/a&gt;.&lt;/p&gt;</description>
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      <title>Stories from old papers</title>
      <link>//fihm.co.uk/posts/old_papers/</link>
      <pubDate>Mon, 11 Jun 2018 01:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/posts/old_papers/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/posts/buckton_aphid.png&#34; alt=&#34;An aphid drawn by George Bowdler Buckton&#34; title=&#34;An aphid drawn by George Bowlder Buckton&#34;&gt;&#xA;&lt;em&gt;Figure: An aphid sketched by George Bowlder Buckton in &amp;lsquo;A monograph of the Membracidæ&amp;rsquo;. Image digitised by the University of Illinois Urbana Champaign, available via the &lt;a href=&#34;https://doi.org/10.5962/bhl.title.34753&#34;&gt;Biodiversity Heritage Library&lt;/a&gt;.&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;Most people&amp;rsquo;s idea of chemistry is of lab-coated scientists mixing liquids, making explosions, causing fires, and growing crystals. Though this stereotype—like most—is based on reality, a key part of any chemistry project is sitting down and reading the ‘literature’: the research papers written by scientists who have worked in the field before you.&#xA;This is, as all researchers know, often quite a mixed experience: once you have located relevant papers and breached the thicket of customised journal websites, the task of reading begins. You have to wade through the many articles that do not quite cover the topics you had thought, struggle past lengthy screeds that emphasise precisely the least interesting part of their work, and have your hopes dashed as you discover your inspired new compound has been already been synthesised.&#xA;Sometimes though, these searches can be an absolute pleasure. This is particularly true of older articles. There is a particular thrill in realising the paper you are reading is not only telling you about the topic in which you are interested, but the world as it was fifty, or even a hundred years ago. For example, imagine what it would be like to be G. S. Zhdanov, determining the structure of zinc cyanide in 1941,&lt;sup id=&#34;fnref:1&#34;&gt;&lt;a href=&#34;#fn:1&#34; class=&#34;footnote-ref&#34; role=&#34;doc-noteref&#34;&gt;1&lt;/a&gt;&lt;/sup&gt; just before the launch of Operation Barbarossa. No matter how exciting the topic of these old papers, they often leave questions completely unanswered: not for any scientific neglect, but because the technical capabilities to solve the problems at hand were simply not available. If you&amp;rsquo;re reading a chemistry paper written before World War I, for example, the authors will not know the structures of their samples because X-ray crystallography had not been invented. The combined technology of over a century of research can make the answers to these historical questions unambiguously straightforward.&#xD;&#xD;My current favourite historical author, George Bowdler Buckton, wrote probably the oldest paper I have consulted in earnest, which was published in 1855. 1855 is, by the standards of chemistry, practically prehistoric: Mendeleev’s periodic table wasn’t presented until fourteen years later, in 1869. As a result, there are some distinctive period features: the mass of nitrogen used is two times too big, and as a result the he described a complicated &amp;lsquo;sulpocyanide&amp;rsquo; molecule (C&lt;sub&gt;2&lt;/sub&gt;NS&lt;sub&gt;2&lt;/sub&gt;&lt;sup&gt;2–&lt;/sup&gt;) rather than the simpler thiocyanate (NCS&lt;sup&gt;–&lt;/sup&gt;).&#xD;&#xD;Though the paper is disadvantaged by being 163 years old, it is otherwise a very careful piece of research. It is thorough in ways we’d never imagine exploring today: &amp;lsquo;[in] common with all the soluble salts to be described, [the compound] has an exceedingly nauseous taste&amp;rsquo;(!). The writing is also of a style and standard not commonly found in modern science. One product is poetically described as &amp;lsquo;a remarkably beautiful substance, thrown down in the form of innumerable golden plates&amp;rsquo;. Despite their beauty, most of the compounds in this paper have never subsequently been investigated, let alone had their structures determined (watch this space).&#xD;&#xD;George Bowlder Buckton is a figure of interest in his own right. He identifies himself as a Fellow of the Linnean Society, and indeed, many of his most lasting contributions are to be found in plant science, rather than chemistry. His most well known contribution to chemistry is being the first person to successfully synthesise dimethyl mercury.&lt;sup id=&#34;fnref:2&#34;&gt;&lt;a href=&#34;#fn:2&#34; class=&#34;footnote-ref&#34; role=&#34;doc-noteref&#34;&gt;2&lt;/a&gt;&lt;/sup&gt; In retrospect this is a substantial achievement, as dimethyl mercury is one of the more infamously toxic compounds; a few drops can kill, and your death can take many months. A quick read of Buckton’s original papers reassures me that he did not try to carry out his usual full taste characterisation of dimethyl mercury, though we can perhaps deduce this from the fact he had a subsequent career as a biologist.&#xA;George Bowdler Buckton had a number of notable relatives, and those of you of the more literary persuasion may have had a twinge of recognition on seeing his middle name. George was named for his uncle, Thomas Bowdler, who is primarily famous for publishing, with his sister Harriet, a nineteenth century edition of Shakespeare in which &amp;rsquo;those words and expressions are omitted which cannot with propriety be read aloud in a Family&amp;rsquo;. This attempt to moderate Shakespeare’s work is usually considered a ridiculous endeavour: Ophelia’s suicide became a drowning accident, and the character of Doll Tearsheet was removed from Henry IV, Part 2 entirely because she is a prostitute. In short, Thomas and Harriet ‘bowdlerized’ the language. Some near contemporaries of the Bowdlers argued that their efforts in making Shakespeare accessible outweighed the errors in excision. The Victorian poet Swinburne said of Thomas that ‘no man ever did better service to Shakespeare than the man who made it possible to put him into the hands of intelligent and imaginative children’.&lt;sup id=&#34;fnref:3&#34;&gt;&lt;a href=&#34;#fn:3&#34; class=&#34;footnote-ref&#34; role=&#34;doc-noteref&#34;&gt;3&lt;/a&gt;&lt;/sup&gt; George Bowdler Buckton may not have put chemistry into the hands of children (luckily), but his story illustrates some of the manifold and exciting ways that scientific literature connects us to the past.&lt;sup id=&#34;fnref:4&#34;&gt;&lt;a href=&#34;#fn:4&#34; class=&#34;footnote-ref&#34; role=&#34;doc-noteref&#34;&gt;4&lt;/a&gt;&lt;/sup&gt;&lt;/p&gt;</description>
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      <title>Low-dimensional quantum magnetism in CuNCS&lt;sub&gt;2&lt;/sub&gt;</title>
      <link>//fihm.co.uk/publications/prb_2018_cuncs2/</link>
      <pubDate>Thu, 26 Apr 2018 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/prb_2018_cuncs2/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/CuNCS2_summary.png&#34; alt=&#34;Structure and magnetic properties of copper(II) thiocyanate&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;&lt;em&gt;Structure and magnetic properties of copper(II) thiocyanate. (a) The structure of Cu(NCS)&lt;sub&gt;2&lt;/sub&gt;. The polymeric chains go into the screen. (b) The low temperature magnetic structure of Cu(NCS)&lt;sub&gt;2&lt;/sub&gt;.&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;In most magnetic materials the magnetic spins stop moving and freeze into an ordered array when cooled down. For some materials, for example iron, this happens at hundreds of degrees Celsius; for others, it can be a fraction of a degree above absolute zero (-273 ºC). However, in spin liquids, the spins never freeze due to the combination of their geometrical arrangement and interactions. These spin liquid phases have many strange properties, for example &amp;lsquo;fractionalisation&amp;rsquo;, where electrons in the crystal behave as if their fundamental properties can be separated into distinct quasiparticles, like &amp;lsquo;holons&amp;rsquo;, which have charge but no spin, and &amp;lsquo;spinons&amp;rsquo;, magnetic but uncharged quasiparticles.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Keep it simple, silicon</title>
      <link>//fihm.co.uk/publications/prb_2017_soap/</link>
      <pubDate>Wed, 14 Jun 2017 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/prb_2017_soap/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/prb_2017_silicon.png&#34; alt=&#34;Amorphous silicon&#34; title=&#34;Left: structural model of amorphous silicon. Right: The electronic energy levels of amorphous silicon&#34;&gt;&#xA;&lt;em&gt;Left: structural model of amorphous silicon. Right: The electronic energy levels of amorphous silicon&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;Amorphous materials, that is, materials which don&amp;rsquo;t have long-range order, are critical for both windows (silica glass) and Windows (amorphous silicon for TFT screens). Despite their technological importance, we still do not fully understand how the structures of amorphous materials relate to their properties. The relative paucity of experimental information available from X-ray and neutron scattering experiments on amorphous materials (in comparison to crystals) makes determination of their structures challenging. Even once we know how the atoms are connected, it is not trivial to explain their resultant properties.&lt;/p&gt;</description>
    </item>
    <item>
      <title>3D-printing: form and substance</title>
      <link>//fihm.co.uk/posts/3dprinting&#43;materials/</link>
      <pubDate>Mon, 01 May 2017 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/posts/3dprinting&#43;materials/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/posts/furcup.jpg&#34; alt=&#34;A fur cup&#34; title=&#34;Object by Meret Oppenheim, 1936&#34;&gt;&#xA;3D printing is widely predicted to be the future of manufacturing, by groups as varied as the excitable fringes of Silicon Valley and the accelerationist left. They believe that everyone will have a 3D printer in their home, just like everyone has (had?) a &amp;lsquo;2D&amp;rsquo; printer, and these printers are going to produce the quotidian objects of our lives. Just as a printer allows you to produce a piece of paper with whatever words or pictures you desire, your desktop 3D printer will produce any arbitrary physical object.&lt;/p&gt;</description>
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    <item>
      <title>3D MOFs to 2D sheets in 1 easy step</title>
      <link>//fihm.co.uk/publications/jacs_2017_uio-67_nanosheets/</link>
      <pubDate>Fri, 31 Mar 2017 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/jacs_2017_uio-67_nanosheets/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/jacs_2017_hcpUiO-67.png&#34; alt=&#34;Conversion of hcp UiO-67 into nanosheets of hxl UiO-67&#34; title=&#34;Conversion of hcp UiO-67 into nanosheets of hxl UiO-67&#34;&gt;&#xA;&lt;em&gt;Figure: Conversion of &lt;strong&gt;hcp&lt;/strong&gt; UiO-67 into nanosheets of &lt;strong&gt;hxl&lt;/strong&gt; UiO-67&lt;/em&gt;&lt;/p&gt;&#xA;&lt;p&gt;In the past decade or so, people have rediscovered the joys of two dimensions – particularly because of remarkable electronic properties of graphene and other related materials. Very thin sheets of nanoporous materials (like zeolites, for example) are extremely interesting because of their potential as catalysts or membranes for chemical separations. Their thinness lets molecules diffuse rapidly through them, but because they retain the small and uniform pores, they can still discriminate between different kinds of guest molecule.&lt;/p&gt;</description>
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    <item>
      <title>Cyanide and magnetism </title>
      <link>//fihm.co.uk/publications/nchem_2016_cyanide/</link>
      <pubDate>Sun, 21 Feb 2016 18:50:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/nchem_2016_cyanide/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/nchem_2016_cyanide.jpg&#34; alt=&#34;AgAu(CN)2 forms a complex structure that can be explained by analogy to magnetic structures&#34; title=&#34;AgAuCN2&#34;&gt;&#xA;Both chemists and physicists try to control interactions in materials to produce unusual and useful states of matter, but usually they make use of very different techniques and for very different kinds of materials.&#xA;In this paper we show that chemists can learn a lot from physicists and hopefully vice versa!&lt;/p&gt;&#xA;&lt;p&gt;We look at the surprisingly complicated structures of some simple metal cyanide compounds, and show that these structures can be explained by using an analogy to the physics of intrinsically disordered &amp;lsquo;frustrated&amp;rsquo; magnets.&#xA;By changing the chemistry in the material, we were therefore able to explore the physics of these frustrated magnets, including quite unusual magnetic states!&lt;/p&gt;</description>
    </item>
    <item>
      <title>A breathing MOF with nano-correlations</title>
      <link>//fihm.co.uk/publications/eur_2016_zrcdc_breathing/</link>
      <pubDate>Fri, 12 Feb 2016 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/eur_2016_zrcdc_breathing/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/eur_2016_zrcdc.png&#34; alt=&#34;Formation of strained nanodomains in ZrCDC MOF&#34; title=&#34;Formation of strained nanodomains in ZrCDC MOF&#34;&gt;&#xA;This work was was result of a collaboration with a number of universities and facilities but particularly the group of Prof. Dirk De Vos at KU Leuven university and with Bart Bueken and Frederik Vermoortele.&lt;/p&gt;&#xA;&lt;p&gt;One of the remarkable features of MOFs is their flexibility - they can show all kinds of unusual behaviour, from negative linear compressibilities to&#xA;The most distinctive behaviour is perhaps breathing - guest triggered transitions between very two structures with very different porosities.&lt;/p&gt;</description>
    </item>
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      <title>Disorder, design and vibrations</title>
      <link>//fihm.co.uk/publications/nc_2016_procrystals/</link>
      <pubDate>Mon, 08 Feb 2016 18:50:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/nc_2016_procrystals/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/nc_2016_procrystal.png&#34; alt=&#34;The &amp;lsquo;procrystal&amp;rsquo; formed by the arrangement of &amp;lsquo;T&amp;rsquo; shapes on a primitive cubic lattice&#34; title=&#34;The &#39;procrystal&#39; formed by the arrangement of &#39;T&#39; shapes on a primitive cubic lattice&#34;&gt;&#xA;Disorder and defects are often thought to be a problem to be solved in materials science - for example, the presence defects and disorder greatly reduces electrical conductivity in crystals.&#xA;In this paper we examine a particular kind of disordered crystals we termed &amp;lsquo;procrystals&amp;rsquo; and showed that these procrystals have properties impossible to replicate in perfectly ordered crystals.&lt;/p&gt;</description>
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    <item>
      <title>Structure of a MOF-derived molecular glass</title>
      <link>//fihm.co.uk/publications/cc_2015_mof_glass/</link>
      <pubDate>Wed, 06 Jan 2016 18:50:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/cc_2015_mof_glass/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/cc_2015_RMC_box.png&#34; alt=&#34;RMC model of zinc triazole phosphate&#34; title=&#34;A model of the zinc triazole phosphate glass, made using reverse Monte Carlo &#34;&gt;&#xA;This work was was result of a collaboration with Kyoto university, particularly with Dr. Daiki Umeyama and Prof. Satoshi Horike.&lt;/p&gt;&#xA;&lt;p&gt;Most of the interest in metal-organic frameworks (MOFs) has focussed on those that are ordered and crystalline.&#xA;Moreover, MOFs typically don&amp;rsquo;t melt when heated, instead decomposing, which means that they can be difficult to form into the shapes needed for useful applications.&#xA;Glass, in contrast, is is incredibly useful because we can form it into very elaborate shapes without introducing any internal boundaries.&lt;/p&gt;</description>
    </item>
    <item>
      <title>The Kitchen as a Laboratory</title>
      <link>//fihm.co.uk/posts/chefstable&#43;laudan/</link>
      <pubDate>Sun, 03 Jan 2016 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/posts/chefstable&#43;laudan/</guid>
      <description>&lt;p&gt; At this time of year my thoughts begin to turn to food, as of course do many other people’s. As a chemist however, I can’t help but think about food from a scientific perspective. One of the most interesting trends, to my mind at least, is the way that food science has come into the public’s consciousness through the high-end cuisine of ‘molecular gastronomy’ — even if, like &lt;a href=&#34;http://luckypeach.com/on-molecular-gastronomy&#34;&gt;cooking science doyen Harold McGee&lt;/a&gt;, I find the name a little daft . I thus really enjoyed the Netflix series “Chef’s Table”, both as a collection of character portraits and as a showcase for really astonishing food. As someone who is unlikely to eat at any of the featured restaurants and thus get a chance to sample the foods for real, I enjoyed the chance to see the creativity of the cooking that is available.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Short introduction to my research</title>
      <link>//fihm.co.uk/posts/introduction/</link>
      <pubDate>Tue, 02 Jun 2015 09:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/posts/introduction/</guid>
      <description>&lt;p&gt;This is a short and personal introduction to my research interests. I have tried to keep it non-technical and as brief as possible. I will be also posting some additional short articles explaining the key concepts in more detail as I go. Hopefully even with pictures!&lt;/p&gt;&#xA;&lt;p&gt;I am a materials chemist. Materials chemistry, like all fields of research, does not have a firm dictionary definition. What I mean by a materials chemist, then, is a chemist who tries to make and understand chemicals that do things: that is, materials with interesting and unusual properties.&lt;/p&gt;</description>
    </item>
    <item>
      <title></title>
      <link>//fihm.co.uk/programs/indicatrix/</link>
      <pubDate>Tue, 28 Apr 2015 18:44:00 +0000</pubDate>
      <guid>//fihm.co.uk/programs/indicatrix/</guid>
      <description></description>
    </item>
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      <title></title>
      <link>//fihm.co.uk/programs/pascal/</link>
      <pubDate>Tue, 28 Apr 2015 18:44:00 +0000</pubDate>
      <guid>//fihm.co.uk/programs/pascal/</guid>
      <description></description>
    </item>
    <item>
      <title></title>
      <link>//fihm.co.uk/programs/pymolpoly/</link>
      <pubDate>Tue, 28 Apr 2015 18:44:00 +0000</pubDate>
      <guid>//fihm.co.uk/programs/pymolpoly/</guid>
      <description></description>
    </item>
    <item>
      <title>Defect-controlled MOF Mechanics</title>
      <link>//fihm.co.uk/publications/pccp_2015_uio_mechanics/</link>
      <pubDate>Fri, 06 Mar 2015 10:00:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/pccp_2015_uio_mechanics/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/pccp_2015_uio.png&#34; alt=&#34;UiO-66(Hf)&#34; title=&#34;UiO-66(Hf) shows defect dependent negative thermal expansion&#34;&gt;&#xA;In our &lt;a href=&#34;//fihm.co.uk/publications/nc_2014_mof_defects&#34;&gt;previous work&lt;/a&gt; we discovered that UiO-66, one of the canonical metal-organic frameworks (MOFs), can contain correlated defects, and showed that we have a degree of synthetic control over the presence and distribution of defects.&lt;/p&gt;&#xA;&lt;p&gt;In this paper we use this control over defects to tune the physical properties of UiO-66. In particular, we look at the thermomechanical properties of UiO-66 - its response to changing temperature - examine how they change with different concentrations of defects.&#xA;We also show that the behaviour of UiO-66 on heating is pretty unusual. First, it rapidly densifies when heated to about 300 &lt;sup&gt;o&lt;/sup&gt;C (as loosely bound molecules are driven off). Second, this densified material exhibits &amp;lsquo;colossal&amp;rsquo; isotropic negative thermal expansion - i.e. when heated it shrinks in every direction.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Flexibility in a ferroelastic MOF</title>
      <link>//fihm.co.uk/publications/cec_2015_ferroelastic_cutcm/</link>
      <pubDate>Sat, 31 Jan 2015 18:50:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/cec_2015_ferroelastic_cutcm/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/cec_2015_cutcm.png&#34; alt=&#34;Cu(tcm)&#34; title=&#34;The structure of Cu tcm as it goes through the ferroelastic phase transition.&#34;&gt;&#xA;One of most exciting features of metal-organic frameworks (MOFs) is their potential to be incredibly flexible.&#xA;In this paper we report a new MOF, copper(I) tricyanomethanide, Cu(tcm) that illustrates this very well.&#xA;Cu(tcm) undergoes a ferroelastic phase transition at T&lt;sub&gt;f&lt;/sub&gt; = 240 K and below this temperature shows thermal expansion an order-of-magnitude larger than above the transition.&#xA;In fact, the low-temperature phase α-Cu(tcm) shows &amp;lsquo;colossal&amp;rsquo; positive and negative thermal expansion that is the strongest ever reported for a framework material.&#xA;We also found that Cu(tcm) can be converted just by exposure to gaseous acetonitrile to another new phase (acetonitrilo-copper(I) tricyanomethanide), and that this reaction can be reversed by putting copper tricyanomethanide under vacuum&#xA;Infrared spectroscopy measurements are sensitive to the phase change, suggesting that Cu(tcm) might perhaps find application in solid-phase acetonitrile sensing.&lt;/p&gt;</description>
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    <item>
      <title>MOF Defect Nanoregions</title>
      <link>//fihm.co.uk/publications/nc_2014_mof_defects/</link>
      <pubDate>Sat, 31 Jan 2015 18:49:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/nc_2014_mof_defects/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/nc_2014_uio66_nanoregions.png&#34; alt=&#34;defect nanoregions in UiO-66(Hf)&#34; title=&#34;Defect nanoregions in UiO-66(Hf)&#34;&gt;&lt;/p&gt;&#xA;&lt;p&gt;The properties of many conventional materials are intimately connected to the presence of correlated defects, including both the solid electrolytes in batteries and high temperature oxide superconductors.&#xA;Although defects have been recently found to exist in MOFs, the prevailing understanding is that these defects are randomly distributed.&#xA;In this paper we show for the first time that defects can be correlated in MOFs and that we can control this defects synthetically.&#xA;This suggests that we might be able to create MOFs that show the same diversity of useful properties as in conventional materials.&lt;/p&gt;</description>
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    <item>
      <title>Negative Area Compressibility</title>
      <link>//fihm.co.uk/publications/cc_2014_nac_agtcm/</link>
      <pubDate>Sat, 31 Jan 2015 18:48:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/cc_2014_nac_agtcm/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/cc_2014_agtcm.png&#34; alt=&#34;Agtcm&#34; title=&#34;Silver tricyanomethanide under pressure&#34;&gt;&#xA;In this paper we report the first known example of a material that shows negative area compressibility , that is a material that expands in two perpendicular directions when compressed hydrostatically (i.e. equally in all directions).&lt;/p&gt;&#xA;&lt;p&gt;This counterintutive property is the result of the layered structure of silver (I) tricyanomethanide, Ag(tcm). Due to the weak forces between the layers it is easy to compress the layers together. This in turn also flattens out the ripples within the layers, causing the crystal to expand in the other two directions.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Parameterising the INVERT approach</title>
      <link>//fihm.co.uk/publications/jpcm_2013_invert2/</link>
      <pubDate>Sat, 31 Jan 2015 18:47:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/jpcm_2013_invert2/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/jpcm_2013_invert2.png&#34; alt=&#34;Parameterisation&#34; title=&#34;The fitting landscape&#34;&gt;&#xA;This paper gives more detail about the &lt;a href=&#34;//fihm.co.uk/publications/PRL_2010_INVERT&#34;&gt;&amp;lsquo;INVERT&amp;rsquo; approach&lt;/a&gt; and outlines both the challenges faced in trying to use data-driven methods for amorphous structural solution and some of the possible solutions to this problem.&lt;/p&gt;&#xA;&lt;p&gt;&lt;em&gt;Figure: Ordinarily, the problem solving the structure of amorphous materials from diffraction data is both underconstrained (there are too many solutions) and taxing to reach (the fitting landscape is poorly shaped). This is shown on the left and is compared to an idealised &amp;rsquo;target&amp;rsquo; landscape on the right.&lt;/em&gt;&lt;/p&gt;</description>
    </item>
    <item>
      <title>Measuring Simplicity</title>
      <link>//fihm.co.uk/publications/pssb_2013_simplicity/</link>
      <pubDate>Sat, 31 Jan 2015 18:46:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/pssb_2013_simplicity/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/pssb_2013_simplicity.png&#34; alt=&#34;Simplicity&#34; title=&#34;A single a-Si configuration, with atoms colored according to 3 measures of their local simplicity.&#34;&gt;&#xA;Quantifying and understanding the structures of amorphous materials can be difficult, because they don&amp;rsquo;t have the long-rage periodicity we rely on to understand the structures of crystals.&#xA;In this paper, we extend the ideas of our &lt;a href=&#34;//fihm.co.uk/publications/PRL_2010_INVERT&#34;&gt;previous work&lt;/a&gt; by introducing the concept of &amp;lsquo;structural simplicity&amp;rsquo; in the context of amorphous materials. We also show that structural simplicity can be quantified, and give two easily calculated geometric measures of simplicity. These methods could prove useful for both understanding and determining the structures of amorphous materials.&lt;/p&gt;</description>
    </item>
    <item>
      <title>A short history of explosives</title>
      <link>//fihm.co.uk/posts/bang_explosives/</link>
      <pubDate>Sat, 31 Jan 2015 18:45:00 +0000</pubDate>
      <guid>//fihm.co.uk/posts/bang_explosives/</guid>
      <description>&lt;p&gt;This is a short article which was published in Oxford&amp;rsquo;s student popular science magazine, &lt;a href=&#34;http://www.bangscience.org/&#34;&gt;Bang!&lt;/a&gt;. See it in its illustrated glory &lt;a href=&#34;http://www.bangscience.org/2012/02/issue-11/&#34;&gt;here&lt;/a&gt; (page 21).&lt;/p&gt;&#xA;&lt;h2 id=&#34;explosives&#34;&gt;Explosives&lt;/h2&gt;&#xA;&lt;p&gt;Ask the average ten-year-old what chemists do, and “make explosions” would probably be the first answer.  As explosions tend to be inconvenient if you are concerned about the structural integrity of your working environment, most chemists try to avoid them.  But what is an explosion?&lt;/p&gt;&#xA;&lt;p&gt;Simply put, it’s the very rapid expansion or release of gas.  Any kind of rapid expansion can cause an explosion, whether from a chemical explosive, the intense heat of a nuclear weapon or from steam, e.g. microwaving an unpierced potato for too long. Explosives, though, are by far the useful way to generate an explosion no matter if you want to fire a gun, demolish a building, or mine.  The power of explosives, for example one gram of RDX, a modern explosive, produces 24000 times its own volume in gas, is down to their chemical structure.&lt;/p&gt;</description>
    </item>
    <item>
      <title>Accelerated aging for making porous MOFs</title>
      <link>//fihm.co.uk/publications/gc_2013_aging2/</link>
      <pubDate>Sat, 31 Jan 2015 18:45:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/gc_2013_aging2/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/gc_2013_aging2.png&#34; alt=&#34;Accelerated aging reaction mixture&#34; title=&#34;An example of a typical reaction&#34;&gt;&#xA;In our &lt;a href=&#34;//fihm.co.uk/publications/cs_2012_aging&#34;&gt;previous work&lt;/a&gt;, we showed that accelerated aging is a practical method for making metal-organic frameworks (MOFs) without needing bulk solvent or high temperatures from cheap and safe starting materials.&#xA;In this paper we demonstrate that it is possible to directly make porous MOFs using accelerated aging. We also extend the chemistry to additional metals.&lt;/p&gt;&#xA;&lt;p&gt;&lt;em&gt;Figure: An example of a typical aging reaction on 10g scale with Canadian penny for scale.&lt;/em&gt;&lt;/p&gt;</description>
    </item>
    <item>
      <title>Bullvalene</title>
      <link>//fihm.co.uk/posts/bang_bullvalene/</link>
      <pubDate>Sat, 31 Jan 2015 18:45:00 +0000</pubDate>
      <guid>//fihm.co.uk/posts/bang_bullvalene/</guid>
      <description>&lt;p&gt;This is a short post based on a &lt;a href=&#34;http://pubs.acs.org/doi/abs/10.1021/ed078p924&#34;&gt;J Chem Ed article&lt;/a&gt;, describing a remarkable hydrocarbon in permanent flux.&#xA;&lt;img src=&#34;//fihm.co.uk/images/posts/BANG_bullvalene.png&#34; alt=&#34;Bullvalene&#34; title=&#34;Structural formula of Bullvalene&#34;&gt;&#xA;&lt;em&gt;Figure: The structural formula of bullvalene - every single carbon atom in the structure will interchange with every other atom at room temperature.&lt;/em&gt;&lt;/p&gt;&#xA;&lt;h2 id=&#34;bullvalene&#34;&gt;Bullvalene&lt;/h2&gt;&#xA;&lt;p&gt;A glance at a line drawing of a molecule might give the impression that molecules are sedate entities, calming drifting through the microscopic world. Molecules are in reality very lively, perpetually vibrating, tumbling and bouncing off each other.  Despite all this motion, bonds in molecules remain intact, as the energy needed to break them is so much larger than the energy of a molecule at room temperature.&lt;/p&gt;</description>
    </item>
    <item>
      <title>NTE &amp; NLC OMG!</title>
      <link>//fihm.co.uk/posts/bang_ntenlc/</link>
      <pubDate>Sat, 31 Jan 2015 18:45:00 +0000</pubDate>
      <guid>//fihm.co.uk/posts/bang_ntenlc/</guid>
      <description>&lt;p&gt;This is a short article which was published in Oxford&amp;rsquo;s student popular science magazine, &lt;a href=&#34;http://www.bangscience.org/&#34;&gt;Bang!&lt;/a&gt;. See it in its illustrated glory &lt;a href=&#34;http://www.bangscience.org/2012/02/issue-10/&#34;&gt;here&lt;/a&gt; (page 20).&lt;/p&gt;&#xA;&lt;p&gt;Things expand when heated and contract when compressed. Obvious – but not always true. In the past fifteen years researchers have produced some striking examples of counterintuitive materials that contract on heating (negative thermal expansion, NTE) or expand in one direction when uniformly compressed  (negative linear compressibility NLC).&lt;/p&gt;</description>
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    <item>
      <title>A webtool for calculating compressibilities &amp; thermal expansion</title>
      <link>//fihm.co.uk/publications/jac_2012_pascal/</link>
      <pubDate>Sat, 31 Jan 2015 18:44:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/jac_2012_pascal/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/jac_2012_PASCal.png&#34; alt=&#34;PASCal&#34; title=&#34;Different unit cell choices will give different responses - only the principal axes give the true response.&#34;&gt;&#xA;This paper describes &lt;a href=&#34;http://pascal.chem.ox.ac.uk&#34;&gt;PASCal&lt;/a&gt;, a simple webtool designed to calculate the principal thermal expansivities or compressibilities of a system from lattice parameters. For low symmetry crystals, the arbitrary choice of unit cell means that if you only look at the cell lengths, it is possible to miss interesting features in the (thermo)mechanical behaviour of a crystal, for example negative thermal expansion or negative compressibilities.&#xA;PASCal is designed to be an easy method for calculating the principal strain values that give the complete description of these systems.&#xA;The paper includes three case-studies where re-analysis using PASCal revealed some extra information about the response of the crystals to changing pressure or temperature.&lt;/p&gt;</description>
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    <item>
      <title>Accelerated aging for making MOFs</title>
      <link>//fihm.co.uk/publications/cs_2012_aging/</link>
      <pubDate>Sat, 31 Jan 2015 18:43:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/cs_2012_aging/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/cs_2012_aging.png&#34; alt=&#34;Accelerated aging&#34; title=&#34;A summary of the accelerated aging reactions&#34;&gt;&#xA;Metal-organic frameworks have the potential to be materials that form a part of a greener economy.&#xA;Laboratory syntheses of MOFs however use high temperatures, large amounts toxic solvents and relatively expensive soluble metal sources.&#xA;If we are ever going to use these materials, therefore, we will need to develop new ways to synthesise them&#xA;In this paper we report a new low-energy method of making MOFs, which we call &amp;lsquo;accelerated aging&amp;rsquo;.&#xA;We show that just by mixing a metal oxide, the organic ligand, and small amount of an ammonium salt catalyst, and leaving the reactants in a warm humid environment for a few days, it is possible to make phase pure MOF.&#xA;The success of these aging reactions also demonstrates the surprising reactivity of MOFs even without bulk solvent.&lt;/p&gt;</description>
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      <title>Amorphous structures from diffraction data?</title>
      <link>//fihm.co.uk/publications/prl_2010_invert/</link>
      <pubDate>Sat, 31 Jan 2015 18:42:00 +0000</pubDate>
      <guid>//fihm.co.uk/publications/prl_2010_invert/</guid>
      <description>&lt;p&gt;&lt;img src=&#34;//fihm.co.uk/images/publications/prl_2010_INVERT_asi.png&#34; alt=&#34;aSi&#34; title=&#34;Three sections of configurations of amorphous silicon.&#34;&gt;&#xA;Despite the importance of disordered materials, we still find it very difficult to determine their structures, because the lack of long-range prevents the use of conventional crystallographic techniques.&#xA;This &amp;rsquo;nanostructure problem&amp;rsquo; as it has been termed, is one of the biggest challenges in the solid state sciences.&#xA;In this paper we show that by making use of the idea of &amp;lsquo;invariant&amp;rsquo; local environments in structure determination - in particular by minimising the variance in local data - it is possible to make significantly better models of amorphous and nanostructured materials.&lt;/p&gt;</description>
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