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    <title>Physics &#187; Ultrafast &amp; Terahertz Photonics: Publications (tag [2018])</title>
    <link>https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/</link>
    <description>The latest from Physics &#187; Ultrafast &amp; Terahertz Photonics: Publications (tag [2018])</description>
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    <category>THz spectroscopy</category>
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    <item>
      <title>Graphene controlled Brewster angle device for ultra broadband terahertz modulation</title>
      <link>https://www.nature.com/articles/s41467-018-07367-8</link>
      <description>&lt;p&gt;Z. Chen, X. Chen, L. Tao, K. Chen, M. Long, K. Yan, R.I. Stantchev, &lt;strong&gt;E. Pickwell-MacPherson&lt;/strong&gt; &amp;amp; J.-B. Xu&lt;br /&gt;
   Nature Communications &lt;strong&gt;9&lt;/strong&gt; 4909 (November 2018) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/Chen_NComms_2018.pdf"&gt;pdf&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="https://www.nature.com/articles/s41467-018-07367-8"&gt; ref &lt;/a&gt;]&lt;/p&gt;

&lt;p&gt;&lt;img src="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/graphene_device-xuequan_chen.jpg?maxWidth=200&amp;amp;maxHeight=160" border="0" alt="Chen 2018" style="float: left; border: 8px solid white;" /&gt;&lt;/p&gt;

&lt;p&gt;Terahertz modulators with high tunability of both intensity and phase are essential for effective control of electromagnetic properties. Due to the underlying physics behind existing approaches there is still a lack of broadband devices able to achieve deep modulation. Here, we demonstrate the effect of tunable Brewster angle controlled by graphene, and develop a highly-tunable solid-state graphene/quartz modulator based on this mechanism. The Brewster angle of the device can be tuned by varying the conductivity of the graphene through an electrical gate. In this way, we achieve near perfect intensity modulation with spectrally flat modulation depth of 99.3 to 99.9 percent and phase tunability of up to 140 degree in the frequency range from 0.5 to 1.6&amp;thinsp;THz. Different from using electromagnetic resonance effects (for example, metamaterials), this principle ensures that our device can operate in ultra-broadband. Thus it is an effective principle for terahertz modulation.&lt;/p&gt;

&lt;div align="left"&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1038/s41467-018-07367-8&amp;amp;httpAccept=image%2Fjpeg&amp;amp;apiKey=23942728d429d8cd622400c4a7485a23" border="0" /&gt;&lt;/div&gt;

&lt;div class="altmetric-embed" data-badge-popover="right" data-badge-type="2" data-doi="10.1038/s41467-018-07367-8" data-hide-no-mentions="true"&gt;&lt;/div&gt;</description>
      <category>THz components</category>
      <category>2018</category>
      <category>nanomaterials</category>
      <category>MacPherson</category>
      <pubDate>Thu, 29 Nov 2018 07:41:00 GMT</pubDate>
      <guid isPermaLink="false">8a1785d8675a41e101675e6a7d2628cd</guid>
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    <item>
      <title>The Effects of Doping Density and Temperature on the Optoelectronic Properties of Formamidinium Tin Triiodide Thin Films</title>
      <link>https://onlinelibrary.wiley.com/doi/10.1002/adma.201804506</link>
      <description>&lt;p&gt;&lt;strong&gt;R. L. Milot&lt;/strong&gt;, M. T. Klug, C. L. Davies, Z. Wang, H. Kraus, H. J. Snaith, M. B. Johnston, and L. M. Herz&lt;br /&gt;
  Advanced Materials (Sept 2018) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/milot_advmater_2018.pdf"&gt;pdf&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="https://onlinelibrary.wiley.com/doi/10.1002/adma.201804506"&gt; ref &lt;/a&gt;]&lt;/p&gt;

&lt;p&gt;&lt;img src="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/fasni3_toc_2.png?maxWidth=222&amp;amp;maxHeight=200" alt="fasni3_toc_2.png" style="float: left; margin-left: 5px; margin-right: 5px;" border="0" /&gt;Optoelectronic properties are unraveled for formamidinium tin triiodide (FASnI&lt;sub&gt;3&lt;/sub&gt;) thin films, whose background hole doping density is varied through SnF&lt;sub&gt;2&lt;/sub&gt; addition during film fabrication. Monomolecular charge&#8208;carrier recombination exhibits both a dopant&#8208;mediated part that grows linearly with hole doping density and remnant contributions that remain under tin&#8208;enriched processing conditions. At hole densities near 10&lt;sup&gt;20&lt;/sup&gt; cm&lt;sup&gt;&#8722;3&lt;/sup&gt;, a strong Burstein&amp;ndash;Moss effect increases absorption onset energies by &#8776;300 meV beyond the bandgap energy of undoped FASnI&lt;sub&gt;3&lt;/sub&gt; (shown to be 1.2 eV at 5 K and 1.35 eV at room temperature). At very high doping densities (10&lt;sup&gt;20&lt;/sup&gt; cm&lt;sup&gt;&#8722;3&lt;/sup&gt;), temperature&#8208;dependent measurements indicate that the effective charge&#8208;carrier mobility is suppressed through scattering with ionized dopants. Once the background hole concentration is nearer 10&lt;sup&gt;19&lt;/sup&gt; cm&lt;sup&gt;&#8722;3&lt;/sup&gt; and below, the charge&#8208;carrier mobility increases with decreasing temperature according to &#8776;&lt;i&gt;T&lt;/i&gt;&lt;sup&gt;&#8722;1.2&lt;/sup&gt;, suggesting that it is limited mostly by intrinsic interactions with lattice vibrations. For the lowest doping concentration of 7.2 &#215; 10&lt;sup&gt;18&lt;/sup&gt; cm&lt;sup&gt;&#8722;3&lt;/sup&gt;, charge&#8208;carrier mobilities reach a value of 67 cm&lt;sup&gt;2&lt;/sup&gt; V&lt;sup&gt;&#8722;1&lt;/sup&gt; s&lt;sup&gt;&#8722;1&lt;/sup&gt; at room temperature and 470 cm&lt;sup&gt;2&lt;/sup&gt; V&lt;sup&gt;&#8722;1&lt;/sup&gt; s&lt;sup&gt;&#8722;1&lt;/sup&gt; at 50 K. Intraexcitonic transitions observed in the THz&#8208;frequency photoconductivity spectra at 5 K reveal an exciton binding energy of only 3.1 meV for FASnI&lt;sub&gt;3&lt;/sub&gt;, in agreement with the low bandgap energy exhibited by this perovskite.&lt;/p&gt;

&lt;div align="left"&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1002/adma.201804506&amp;amp;httpAccept=image%2Fjpeg&amp;amp;apiKey=23942728d429d8cd622400c4a7485a23" border="0" /&gt;&lt;/div&gt;

&lt;div class="altmetric-embed" data-badge-popover="right" data-badge-type="2" data-doi="10.1002/adma.201804506" data-hide-no-mentions="true"&gt;&lt;/div&gt;</description>
      <category>THz spectroscopy</category>
      <category>2018</category>
      <category>photoluminescence</category>
      <category>Milot</category>
      <category>perovskites</category>
      <pubDate>Thu, 20 Sep 2018 14:18:00 GMT</pubDate>
      <guid isPermaLink="false">8a1785d865e8039f0165f7587ae07ffc</guid>
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      <title>Efficient Intraband Hot Carrier Relaxation in the Perovskite Semiconductor Cs&lt;sub&gt;1-x&lt;/sub&gt;Rb&lt;sub&gt;x&lt;/sub&gt;SnI&lt;sub&gt;3&lt;/sub&gt; Mediated by Strong Electron-Phonon Coupling</title>
      <link>https://pubs.acs.org/doi/10.1021/acs.jpcc.8b07792</link>
      <description>&lt;p&gt;&lt;strong&gt;M. Monti&lt;/strong&gt;, S. Tao, &lt;strong&gt;M. Staniforth&lt;/strong&gt;, &lt;strong&gt;A. Crocker, E. Griffin&lt;/strong&gt;, A. Wijesekara, R.A. Hatton, and&lt;strong&gt; J. Lloyd-Hughes&lt;/strong&gt;&lt;br /&gt;
   J. Phys. Chem. C &lt;strong&gt;&lt;span class="citation_volume"&gt;122&lt;/span&gt;&lt;/strong&gt; 20669 (Aug 2018) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/monti2018.pdf"&gt;pdf&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="https://pubs.acs.org/doi/10.1021/acs.jpcc.8b07792"&gt; ref &lt;/a&gt;]&lt;/p&gt;

&lt;p&gt;&lt;img src="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/monti2018.png?maxWidth=250&amp;amp;maxHeight=187" border="0" alt="THz conductivity dynamics of GaAs and CsSni3" style="float: left;" /&gt;The dynamic increase in THz photoconductivity resulting from energetic intraband relaxation was used to track the formation of highly mobile charges in thin films of the tin iodide perovskite Cs&lt;sub&gt;1-x&lt;/sub&gt;Rb&lt;sub&gt;x&lt;/sub&gt;SnI&lt;sub&gt;3&lt;/sub&gt;, with x=0 and x=0.1. Energy relaxation times were found to be around 500fs, comparable to those in the prototypical inorganic semiconductor GaAs. At low excess energies the efficient intraband energy relaxation in the lowest conduction and valence bands of Cs&lt;sub&gt;1-x&lt;/sub&gt;Rb&lt;sub&gt;x&lt;/sub&gt;SnI&lt;sub&gt;3&lt;/sub&gt; can be understood within the context of the Fr&#246;hlich electron-phonon interaction, with a strong coupling strength. For higher excess energies the photoconductivity rise time lengthens in accordance with carrier injection into multiple bands, identified by quantitative first-principles bandstructure calculations and photoluminescence spectroscopy. The findings contribute to the development of design rules for photovoltaic devices capable of extracting hot carriers from perovskite semiconductors.&lt;/p&gt;

&lt;div align="left"&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1021/acs.jpcc.8b07792&amp;amp;httpAccept=image%2Fjpeg&amp;amp;apiKey=23942728d429d8cd622400c4a7485a23" border="0" /&gt;&lt;/div&gt;

&lt;div class="altmetric-embed" data-badge-popover="right" data-badge-type="2" data-doi="10.1021/acs.jpcc.8b07792" data-hide-no-mentions="true"&gt;&lt;/div&gt;</description>
      <category>THz spectroscopy</category>
      <category>2018</category>
      <category>photoluminescence</category>
      <category>perovskites</category>
      <category>Lloyd-Hughes</category>
      <pubDate>Tue, 21 Aug 2018 08:45:00 GMT</pubDate>
      <guid isPermaLink="false">8a1785d76533e34d01655ba9150a4f34</guid>
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    <item>
      <title>Highly Sensitive Terahertz Thin-Film Total Internal Reflection Spectroscopy Reveals in Situ Photoinduced Structural Changes in Methylammonium Lead Halide Perovskites</title>
      <link>https://pubs.acs.org/doi/10.1021/acs.jpcc.8b05695</link>
      <description>&lt;p&gt;&lt;strong&gt;Q. Sun&lt;/strong&gt;, X. Liu, J. Cao, R.I. Stantchev, Y. Zhou, X. Chen, E.P.J. Parrott, &lt;strong&gt;J. Lloyd-Hughes&lt;/strong&gt;, N. Zhao, and &lt;strong&gt;E. Pickwell-MacPherson&lt;/strong&gt;&lt;br /&gt;
   J. Phys. Chem. C &lt;strong&gt;122&lt;/strong&gt; 17552 (June 2018) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/sun2018.pdf"&gt;pdf&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="https://pubs.acs.org/doi/10.1021/acs.jpcc.8b05695"&gt; ref &lt;/a&gt;]&lt;/p&gt;

&lt;p&gt;&lt;img src="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/jp-2018-056952_0006.gif" border="0" alt="Sun 2018" width="207" height="200" style="float: left; border: 8px solid white;" /&gt;&lt;/p&gt;

&lt;p&gt;Terahertz (THz) thin-film total internal reflection (TF-TIR) spectroscopy is shown to have an enhanced sensitivity to the vibrational properties of thin films in comparison with standard THz transmission spectroscopy. This increased sensitivity was used to track photoinduced modifications to the structure of thin films of methylammonium (MA) lead halide, MAPbI&lt;sub&gt;3&amp;ndash;&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Br&lt;sub&gt;&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt; (&lt;i&gt;x&lt;/i&gt; = 0, 0.5, 1, and 3). Initially, illumination strengthened the phonon modes around 2 THz, associated with Pb&amp;ndash;I stretch modes coupled to the MA ions, whereas the 1 THz twist modes of the inorganic octahedra did not alter in strength. Under longer term illumination, the 1 THz phonon modes of encapsulated films slowly reduced in strength, whereas in films exposed to moisture and oxygen, these phonons weaken more rapidly and blue-shift in frequency. The rapid monitoring of environmentally induced changes to the vibrational modes afforded by TF-TIR spectroscopy offers applications in the characterization and quality control of the perovskite thin-film solar cells and other thin-film semiconductors.&lt;/p&gt;

&lt;div class="altmetric-embed" data-badge-popover="right" data-badge-type="2" data-doi="10.1021/acs.jpcc.8b05695" data-hide-no-mentions="true"&gt;&lt;/div&gt;

&lt;div&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1021/acs.jpcc.8b05695&amp;amp;httpAccept=image%2Fjpeg&amp;amp;apiKey=23942728d429d8cd622400c4a7485a23" border="0" /&gt;&lt;/div&gt;</description>
      <category>THz spectroscopy</category>
      <category>2018</category>
      <category>MacPherson</category>
      <category>perovskites</category>
      <category>Lloyd-Hughes</category>
      <pubDate>Mon, 06 Aug 2018 12:51:00 GMT</pubDate>
      <guid isPermaLink="false">8a17841a64fa310601650f4a8eb416d6</guid>
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      <title>Cs&lt;sub&gt;1&#8722;x&lt;/sub&gt;Rb&lt;sub&gt;x&lt;/sub&gt;SnI&lt;sub&gt;3&lt;/sub&gt; light harvesting semiconductors for perovskite photovoltaics</title>
      <link>https://dx.doi.org/10.1039/C8QM00159F</link>
      <description>&lt;p&gt;K.P. Marshall, S. Tao, M. Walker, D.S. Cook, &lt;strong&gt;J. Lloyd-Hughes&lt;/strong&gt;, S. Varagnolo, A. Wijesekara, D. Walker, R.I. Walton and R.A. Hatton&lt;br /&gt;
   Materials Chemistry Frontiers &lt;span class="list__item-data"&gt;&lt;strong&gt;2&lt;/strong&gt;:1515 &lt;/span&gt;(June 2018) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/marshall2018.pdf"&gt;pdf&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="https://dx.doi.org/10.1039/C8QM00159F"&gt; ref &lt;/a&gt;]&lt;/p&gt;

&lt;p&gt;&lt;img src="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/marshall2018.gif" border="0" alt="marshall2018.gif" style="float: left;" /&gt;&lt;/p&gt;

&lt;p&gt;We show that films of the 3-dimensional perovskite Cs&lt;small&gt;&lt;sub&gt;1&#8722;&lt;em&gt;x&lt;/em&gt;&lt;/sub&gt;&lt;/small&gt;Rb&lt;small&gt;&lt;sub&gt;&lt;em&gt;x&lt;/em&gt;&lt;/sub&gt;&lt;/small&gt;SnI&lt;small&gt;&lt;sub&gt;3&lt;/sub&gt;&lt;/small&gt; can be prepared from room temperature &lt;em&gt;N&lt;/em&gt;,&lt;em&gt;N&lt;/em&gt;-dimethylformamide solutions of RbI, CsI and SnCl&lt;small&gt;&lt;sub&gt;2&lt;/sub&gt;&lt;/small&gt; for &lt;em&gt;x&lt;/em&gt; &#8804; 0.5, and that for &lt;em&gt;x&lt;/em&gt; &#8804; 0.2 film stability is sufficient for utility as the light harvesting layer in inverted photovoltaic (PV) devices. Electronic absorption and photoluminescence spectroscopy measurements supported by computational simulation, show that increasing &lt;em&gt;x&lt;/em&gt; increases the band gap, due to distortion of the lattice of SnI&lt;small&gt;&lt;sub&gt;6&lt;/sub&gt;&lt;/small&gt; octahedra that occurs when Cs is substituted with Rb, although it also reduces the stability towards decomposition. When Cs&lt;small&gt;&lt;sub&gt;0.8&lt;/sub&gt;&lt;/small&gt;Rb&lt;small&gt;&lt;sub&gt;0.2&lt;/sub&gt;&lt;/small&gt;SnI&lt;small&gt;&lt;sub&gt;3&lt;/sub&gt;&lt;/small&gt; perovskite is incorporated into the model inverted PV device structure; ITO|perovskite|C&lt;small&gt;&lt;sub&gt;60&lt;/sub&gt;&lt;/small&gt;|bathocuproine|Al, an &#8764;120 mV increase in open-circuit is achieved which is shown to correlate with an increase in perovskite ionisation potential. However, for this low Rb loading the increase in band gap is very small (&#8764;30 meV) and so a significant increase in open circuit-voltage is achieved without reducing the range of wavelengths over which the perovskite can harvest light. The experimental findings presented are shown to agree well with the predictions of density functional theory (DFT) simulations of the stability and electronic structure, also performed as part of this study.&lt;/p&gt;

&lt;div align="left"&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1039/C8QM00159F&amp;amp;httpAccept=image%2Fjpeg&amp;amp;apiKey=23942728d429d8cd622400c4a7485a23" border="0" /&gt;&lt;/div&gt;

&lt;div class="altmetric-embed" data-badge-popover="right" data-badge-type="2" data-doi="10.1039/C8QM00159F" data-hide-no-mentions="true"&gt;&lt;/div&gt;</description>
      <category>2018</category>
      <category>photoluminescence</category>
      <category>perovskites</category>
      <category>Lloyd-Hughes</category>
      <pubDate>Wed, 13 Jun 2018 11:34:00 GMT</pubDate>
      <guid isPermaLink="false">8a17841a63d087630163f8ed1a1c5bf2</guid>
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    <item>
      <title>Conduction properties of thin films from a water soluble carbon nanotube/hemicellulose complex</title>
      <link>http://iopscience.iop.org/article/10.1088/1361-6528/aaabd1</link>
      <description>&lt;p&gt;D. Shao, P. Yotprayoonsak, V. Saunajoki, M. Ahlskog, J. Virtanen, V. Kangas, A. Volodin, C. Van Haesendonck, &lt;strong&gt;M. Burdanova, C. D. W. Mosley &lt;/strong&gt;and&lt;strong&gt; J. Lloyd-Hughes&lt;/strong&gt;&lt;br /&gt;
   Nanotechnology &lt;b&gt;29&lt;/b&gt; 145203 (Feb 2018) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/Shao2018.pdf"&gt;pdf&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="http://iopscience.iop.org/article/10.1088/1361-6528/aaabd1"&gt; ref &lt;/a&gt;]&lt;/p&gt;

&lt;p&gt;&lt;img src="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/summaryfigure.png?maxWidth=250" border="0" alt="Complex THz conductivity of a 130nm thick DWNT/xylan composite" style="float: left;" /&gt;We have examined the conductive properties of a carbon nanotube (CNT) based thin film, which were prepared via dispersion in water by non-covalent functionalization of the nanotubes with xylan, a type of hemicellulose. Measurements of low temperature conductivity, Kelvin Probe Force Microscopy, and high frequency (THz) conductivity elucidated the intra-tube and inter-tube charge transport processes in this material. The measurements show excellent conductive properties of the as prepared thin films, with bulk conductivity up to 2000 S/cm. The transport results demonstrate that the hemicellulose does not seriously interfere with the inter-tube conductance.&lt;/p&gt;

&lt;div align="left"&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1088/1361-6528/aaabd1&amp;amp;httpAccept=image%2Fjpeg&amp;amp;apiKey=23942728d429d8cd622400c4a7485a23" border="0" /&gt;&lt;/div&gt;

&lt;div class="altmetric-embed" data-badge-popover="right" data-badge-type="2" data-doi="10.1088/1361-6528/aaabd1" data-hide-no-mentions="true"&gt;&lt;/div&gt;</description>
      <category>THz spectroscopy</category>
      <category>2018</category>
      <category>nanomaterials</category>
      <category>Lloyd-Hughes</category>
      <pubDate>Tue, 06 Feb 2018 13:50:00 GMT</pubDate>
      <guid isPermaLink="false">8a17841a6165d83901616b6249e6484c</guid>
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      <title>Tracking a hysteretic and disorder-broadened phase transition via the electromagnon response in improper ferroelectrics</title>
      <link>http://iopscience.iop.org/article/10.1088/1361-6463/aaa836</link>
      <description>&lt;div class="news-thumbnail" style="float: left; margin-right: 10px; margin-bottom: 5px;"&gt;&lt;img class="thumbnail" width="100" height="100" src="https://warwick.ac.uk/sitebuilder2/file/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications?sbrPage=%2Ffac%2Fsci%2Fphysics%2Fresearch%2Fcondensedmatt%2Fultrafastphotonics%2Fpublications&amp;newsItem=8a17841a60fe7411016103244ed06461" alt="image"&gt;&lt;/div&gt;&lt;p&gt;&lt;strong&gt;C. D. W. Mosley&lt;/strong&gt;, D. Prabhakaran and &lt;strong&gt;J. Lloyd-Hughes&lt;/strong&gt;&lt;br /&gt;
   J. Phys. D: Applied Physics &lt;b&gt;51&lt;/b&gt; 084002 (Jan 2018) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/mosley-2018-jphysd.pdf" target="_blank"&gt;pdf&lt;/a&gt; ][ &lt;a style="text-decoration: none;" href="http://iopscience.iop.org/article/10.1088/1361-6463/aaa836"&gt; ref &lt;/a&gt;]&lt;/p&gt;

&lt;p&gt;We demonstrate that &lt;img src="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/cuznohysteresis.png?maxWidth=300" border="0" alt="Hysteresis in the electromagnon oscillator strength in CuZnO" style="float: left;" /&gt;electromagnons can be used to directly probe the nature of a phase transition between magnetically ordered phases in an improper ferroelectric. The antiferromagnetic/paraelectric to antiferromagnet/ferroelectric phase transition in Cu&lt;sub&gt;1-x&lt;/sub&gt;Zn&lt;sub&gt;x&lt;/sub&gt;O (x = 0, 0.05) alloys was tracked via the electromagnon response using terahertz time-domain spectroscopy, on heating and cooling through the phase transition. The transition was found to exhibit thermal hysteresis, confirming its first-order nature, and to broaden under the influence of spin-disorder upon Zn substitution. The energy of the electromagnon increases upon alloying, as a result of the non-magnetic ions modifying the magnetic interactions that give rise to the multiferroic phase and electromagnons. We describe our findings in the context of recent theoretical work that examined improper ferroelectricity and electromagnons in CuO from phenomenological and first-principles approaches.&lt;/p&gt;

&lt;div class="altmetric-embed" data-badge-popover="right" data-badge-type="2" data-doi="10.1088/1361-6463/aaa836" data-hide-no-mentions="true"&gt;&lt;/div&gt;

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      <category>THz spectroscopy</category>
      <category>2018</category>
      <category>Lloyd-Hughes</category>
      <pubDate>Wed, 17 Jan 2018 08:02:00 GMT</pubDate>
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