<?xml version="1.0" encoding="UTF-8"?>
<?xml-stylesheet href="/static_war/render/xsl/rss2.xsl" media="screen" type="text/xsl"?>
<rss version="2.0">
  <channel>
    <title>Physics &#187; Ultrafast &amp; Terahertz Photonics: Publications (tag [2018,2019])</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 [2018,2019])</description>
    <language>en-GB</language>
    <copyright>(C) 2026 University of Warwick</copyright>
    <lastBuildDate>Tue, 28 Apr 2026 12:37:45 GMT</lastBuildDate>
    <docs>http://blogs.law.harvard.edu/tech/rss</docs>
    <generator>SiteBuilder2, University of Warwick, http://go.warwick.ac.uk/sitebuilder</generator>
    <category>2016</category>
    <category>2017</category>
    <category>2018</category>
    <category>2019</category>
    <category>2020</category>
    <category>2021</category>
    <category>2022</category>
    <category>2023</category>
    <category>2024</category>
    <category>2025</category>
    <category>2026</category>
    <category>biomedical</category>
    <category>highlight</category>
    <category>Lloyd-Hughes</category>
    <category>MacPherson</category>
    <category>Milot</category>
    <category>nanomaterials</category>
    <category>perovskites</category>
    <category>photoluminescence</category>
    <category>review</category>
    <category>semiconductors</category>
    <category>THz components</category>
    <category>THz imaging</category>
    <category>THz spectroscopy</category>
    <category>ultrafast</category>
    <category>Untagged</category>
    <item>
      <title>A Robust Protocol for In Vivo THz Skin Measurements</title>
      <link>https://doi.org/10.1007/s10762-019-00619-8</link>
      <description>&lt;p&gt;&lt;strong&gt;H. Lindley-Hatcher, A. I Hernandez-Serrano, Q. Sun, &lt;/strong&gt;J. Wang, J. Cebrian, L. Blasco, &lt;strong&gt;E. Pickwell-MacPherson&lt;/strong&gt;&lt;br /&gt;
  J Infrared Milli Terahz Waves &lt;strong&gt;40&lt;/strong&gt; 980 (August 2019) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/Lindley-Hatcher2019.pdf"&gt;pdf&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="https://doi.org/10.1007/s10762-019-00619-8"&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/circuit_diagram.png?maxWidth=200" alt="Method" align="left" border="0" /&gt;This work presents an experimental setup to control the way in which pressure interferes with the repeatability of in vivo THz skin measurements. By integrating a pressure sensor circuit into our THz system, it is possible to identify which measurements were taken within a previously specified pressure range. The live response of the pressure sensor helps to acquire data within the desired pressure leading to greater consistency of data between measurements. Additionally, a protocol is proposed to help achieve repeatable results and to remove the effects of the natural variation of the skin through the course of the day. This technique has been shown to be able to quantify the changes induced in the skin following the application of a moisturising skin product and shows the measured result to be significantly different from natural skin variation. This research therefore prepares the way for further studies on the effectiveness of different skin products using in vivo THz measurements.&lt;/p&gt;

&lt;div class="altmetric-embed" data-badge-popover="right" data-badge-type="2" data-doi="10.1007/s10762-019-00619-8" data-hide-no-mentions="true"&gt;&lt;/div&gt;

&lt;div&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1007/s10762-019-00619-8&amp;amp;httpAccept=image%2Fjpeg&amp;amp;apiKey=23942728d429d8cd622400c4a7485a23" border="0" /&gt;&lt;/div&gt;</description>
      <category>THz spectroscopy</category>
      <category>MacPherson</category>
      <category>2019</category>
      <category>biomedical</category>
      <pubDate>Wed, 28 Aug 2019 08:00:00 GMT</pubDate>
      <guid isPermaLink="false">8a17841b6d3ecc05016d71e2f927376d</guid>
    </item>
    <item>
      <title>Ionic liquid gated carbon nanotube saturable absorber for switchable pulse generation</title>
      <link>https://doi.org/10.1021/acs.nanolett.9b01012</link>
      <description>&lt;p&gt;Y. Gladush, A. Mkrtchyan, D. Kopylova, A. Ivanenko, B. Nyushkov, S. Kobtsev, A. Kokhanovskiy, A. Khegai, M. Melkumov, &lt;strong&gt;M.G. Burdanova&lt;/strong&gt;, &lt;strong&gt;M. Staniforth&lt;/strong&gt;, &lt;strong&gt;J. Lloyd-Hughes&lt;/strong&gt; and A.G. Nasibulin&lt;br /&gt;
  Nano Letters &lt;strong&gt;&lt;span class="citation_volume"&gt;19 &lt;/span&gt;&lt;/strong&gt;&lt;span class="citation_volume"&gt;5836&lt;/span&gt;&lt;strong&gt;&lt;span class="citation_volume"&gt;&lt;/span&gt;&lt;/strong&gt; (Aug 2019) [ &lt;a href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/Gladush2019.pdf"&gt;pdf&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="https://doi.org/10.1021/acs.nanolett.9b01012"&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/gladush2019.png?maxWidth=200" alt="Ionic liquid gated carbon nanotube saturable absorber" border="0" align="left" /&gt;Materials with electrically tunable optical properties offer a wide range of opportunities for photonic applications. The optical properties of the single-walled carbon nanotubes (SWCNTs) can be significantly altered in the near infrared region by means of electrochemical doping. The states&#8217; filling, which is responsible for the optical absorption suppression under doping, also alters the nonlinear optical response of the material. Here, for the first time, we report that the electrochemical doping can tailor the nonlinear optical absorption of SWCNT films and demonstrate its application to control pulsed fiber laser generation. With a pump-probe technique we show that under an applied voltage below 2 V the photo-bleaching of the material can be gradually reduced and even turned to photo-induced absorption. Furthermore, we integrated a carbon nanotube electrochemical cell on a side-polished fiber to tune the absorption saturation and implemented it into the fully polarization-maintaining fiber laser. We show that the pulse generation regime can be reversibly switched between femtosecond mode locking and microsecond Q-switching using different gate voltages. This approach paves the road towards carbon nanotube optical devices with tunable nonlinearity.&lt;/p&gt;

&lt;div align="left"&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1021/acs.nanolett.9b01012&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.nanolett.9b01012" data-hide-no-mentions="true"&gt;&lt;/div&gt;</description>
      <category>nanomaterials</category>
      <category>Lloyd-Hughes</category>
      <category>2019</category>
      <pubDate>Thu, 01 Aug 2019 23:10:00 GMT</pubDate>
      <guid isPermaLink="false">8a1785d86c4842b6016c4f72bc614605</guid>
    </item>
    <item>
      <title>Scalable interdigitated photoconductive emitters for the electrical modulation of terahertz beams with arbitrary linear polarization</title>
      <link>https://aip.scitation.org/doi/10.1063/1.5086428</link>
      <description>&lt;p&gt;&lt;strong&gt;C.D.W. Mosley&lt;/strong&gt;, &lt;strong&gt;M. Staniforth&lt;/strong&gt;, &lt;strong&gt;A. I. Hernandez Serrano&lt;/strong&gt;, &lt;strong&gt;E. Pickwell-MacPherson&lt;/strong&gt; and&lt;strong&gt; J. Lloyd-Hughes&lt;/strong&gt;&lt;br /&gt;
  AIP Advances &lt;b&gt;9&lt;/b&gt;, 045323 (Apr 2019) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/mosley2019.pdf" target="_blank" rel="noopener"&gt;pdf&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="https://aip.scitation.org/doi/10.1063/1.5086428" target="_blank" rel="noopener"&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/mosley2019.png?maxWidth=200" alt="" style="margin-right: 10px;" border="0" align="left" /&gt;A multi-element interdigitated photoconductive emitter for broadband THz polarization rotation is proposed and experimentally verified. The device consists of separate pixels for the emission of horizontally and vertically polarized THz radiation. The broadband (0.3&amp;ndash;5.0 THz) nature of the device is demonstrated, and the polarization angle of the generated far-field THz radiation is shown to be readily controlled by varying the relative bias voltage applied to the horizontally and vertically emitting pixels. The device is scalable in design, and with its simple method of polarization rotation it allows the modulation of the generated THz polarization at rates significantly faster than those achievable in ellipsometry systems based on mechanically rotating components.&lt;/p&gt;

&lt;div align="left"&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1063/1.5086428&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="10.1063/1.5086428" data-hide-no-mentions="true"&gt;&lt;/div&gt;</description>
      <category>THz components</category>
      <category>MacPherson</category>
      <category>Lloyd-Hughes</category>
      <category>2019</category>
      <pubDate>Fri, 26 Apr 2019 18:08:00 GMT</pubDate>
      <guid isPermaLink="false">8a17841a6a5500c7016a5ad53c1a2350</guid>
    </item>
    <item>
      <title>Utilizing multilayer structures to enhance terahertz characterization of thin films ranging from aqueous solutions to histology slides</title>
      <link>https://doi.org/10.1364/OL.44.002149</link>
      <description>&lt;p&gt;&lt;strong&gt;Q. Sun,&lt;/strong&gt; K. Liu, X. Chen, X. Liu, A.&lt;strong&gt; I Hernandez-Serrano, &lt;/strong&gt;&lt;strong&gt;E. Pickwell-MacPherson&lt;/strong&gt;&lt;br /&gt;
  Optics Letters &lt;strong&gt;44&lt;/strong&gt; 2149 (April 2019) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/Sun2019.pdf"&gt;pdf&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="https://doi.org/10.1364/OL.44.002149"&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/sun2019.jpeg" alt="Geometry" align="left" border="0" /&gt;We propose a multilayer geometry to characterize thin-film samples in reflection terahertz time domain spectroscopy. Theory indicates that this geometry has higher sensitivity compared to ordinary transmission or reflection geometries when characterizing both low- and high-absorption samples. Pure water and water&amp;ndash;ethanol mixtures are measured to verify the characterization accuracy of the proposed geometry and its capability to measure trace liquids. Paraffin-embedded oral cancer tissue is imaged to further show how the proposed geometry enhances the sensitivity for solid low-absorptive films.&lt;/p&gt;

&lt;div class="altmetric-embed" data-badge-popover="right" data-badge-type="2" data-doi="10.1364/OL.44.002149" data-hide-no-mentions="true"&gt;&lt;/div&gt;

&lt;div&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1364/OL.44.002149&amp;amp;httpAccept=image%2Fjpeg&amp;amp;apiKey=23942728d429d8cd622400c4a7485a23" border="0" /&gt;&lt;/div&gt;</description>
      <category>THz spectroscopy</category>
      <category>THz components</category>
      <category>MacPherson</category>
      <category>2019</category>
      <category>biomedical</category>
      <pubDate>Wed, 17 Apr 2019 16:00:00 GMT</pubDate>
      <guid isPermaLink="false">8a1785d7705d7edd0170c1940aa26fe7</guid>
    </item>
    <item>
      <title>Design and fabrication of 3-D printed conductive polymer structures for THz polarization control</title>
      <link>https://www.osapublishing.org/oe/abstract.cfm?uri=oe-27-8-11635</link>
      <description>&lt;p&gt;&lt;strong&gt;A.I. Hernandez-Serrano&lt;/strong&gt;, &lt;strong&gt;Q. Sun&lt;/strong&gt;, E.G. Bishop, E.R. Griffiths, C.P. Purssel, S.J. Leigh, &lt;strong&gt;J. Lloyd-Hughes &lt;/strong&gt;and &lt;strong&gt;E. Pickwell-MacPherson&lt;/strong&gt;&lt;br /&gt;
  Optics Express &lt;strong&gt;27&lt;/strong&gt; 8 11635 (April 2019) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/hernandez-serrano2019.pdf"&gt;pdf&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="https://www.osapublishing.org/oe/abstract.cfm?uri=oe-27-8-11635"&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/arturo2019.jpg?maxWidth=150&amp;amp;maxHeight=150" alt="arturo2019.jpg" border="0" align="left" /&gt;&lt;/p&gt;

&lt;p&gt;In this paper, we numerically and experimentally demonstrate the inverse polarization effect in three-dimensional (3-D) printed polarizers for the frequency range of 0.5 - 2.7 THz. The polarizers simply consist of 3-D printed strip lines of conductive polylactic acid (CPLA, Proto-Pasta) and do not require a substrate or any further metallic deposition. The experimental and numerical results show that the proposed structure acts as a broadband polarizer between the range of 0.3 THz to 2.7 THz, in which the inverse polarization effect is clearly seen for frequencies above 0.5 THz. In the inverse polarization effect, the transmission of the transverse electric (TE) component exceeds that of the TM component, in contrast to the behavior of a typical wire-grid polarizer. We show how the performance of the polarizers depends on the spacing and thickness of the CPLA structure; extinction ratios higher than 20 dB are achieved. This is the first report using CPLA to fabricate THz polarizers, demonstrating the potential of using conductive polymers to design THz components efficiently and robustly.&lt;/p&gt;

&lt;div class="altmetric-embed" data-badge-popover="right" data-badge-type="2" data-doi="10.1364/OE.27.011635" data-hide-no-mentions="true"&gt;&lt;/div&gt;

&lt;div&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1364/OE.27.011635&amp;amp;httpAccept=image%2Fjpeg&amp;amp;apiKey=23942728d429d8cd622400c4a7485a23" border="0" /&gt;&lt;/div&gt;</description>
      <category>THz components</category>
      <category>MacPherson</category>
      <category>Lloyd-Hughes</category>
      <category>2019</category>
      <pubDate>Thu, 11 Apr 2019 15:40:10 GMT</pubDate>
      <guid isPermaLink="false">8a17841a6a06f00c016a0d0e6ee55aac</guid>
    </item>
    <item>
      <title>Giant negative terahertz photoconductivity in controllably doped carbon nanotube networks</title>
      <link>https://pubs.acs.org/doi/10.1021/acsphotonics.9b00138</link>
      <description>&lt;p&gt;&lt;strong&gt;M.G. Burdanova&lt;/strong&gt;, A.P. Tsapenko, D.A. Satco, R.J. Kashtiban, &lt;strong&gt;C.D.W. Mosley&lt;/strong&gt;, &lt;strong&gt;M. Monti&lt;/strong&gt;, &lt;strong&gt;M. Staniforth&lt;/strong&gt;, J. Sloan, Y. Gladush, A.G. Nasibulin and&lt;strong&gt; J. Lloyd-Hughes&lt;/strong&gt;&lt;br /&gt;
  ACS Photonics &lt;strong&gt;&lt;span class="citation_volume"&gt;6&lt;/span&gt;&lt;/strong&gt; 1058&lt;strong&gt;&lt;span class="citation_volume"&gt;&lt;/span&gt;&lt;/strong&gt; (Mar 2019) [ &lt;a style="text-decoration: none;" href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/burdanova2019.pdf" target="_blank" rel="noopener"&gt;preprint pdf&lt;/a&gt; ] [ &lt;a href="https://warwick.ac.uk/fac/sci/physics/research/condensedmatt/ultrafastphotonics/publications/burdanova2019_si.pdf" target="_blank" rel="noopener"&gt;supplemental info&lt;/a&gt; ] [ &lt;a style="text-decoration: none;" href="https://pubs.acs.org/doi/10.1021/acsphotonics.9b00138" target="_blank" rel="noopener"&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/burdanova2019.jpg?maxWidth=200&amp;amp;maxHeight=156" alt="Negative photoconductivity in carbon nanotubes" border="0" align="left" /&gt;A strong negative photoconductivity was identified in thin film networks of single-walled carbon nanotubes using optical pump, THz probe spectroscopy. The films were controllably doped, using either adsorption doping with different p-type dopant concentrations, or ambipolar doping using an ionic gate. While doping enhanced the THz conductivity and increased the momentum scattering rate, interband photoexcitation lowered the spectral weight and reduced the momentum scattering rate. This negative THz photoconductivity was observed for all doping levels, regardless of the chemical potential, and decayed within a few picoseconds. The strong many-body interactions inherent to these 1D conductors led to trion formation under photoexcitation, lowering the overall conductivity of the carbon nanotube network. The large amplitude of negative THz photoconductivity and the tunability of its recovery time with doping offer promise for spectrally wide-band ultrafast devices including THz detectors, polarizers and modulators.&lt;/p&gt;

&lt;div align="left"&gt;&lt;img src="https://api.elsevier.com/content/abstract/citation-count?doi=10.1021/acsphotonics.9b00138&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/acsphotonics.9b00138" data-hide-no-mentions="true"&gt;&lt;/div&gt;</description>
      <category>THz spectroscopy</category>
      <category>nanomaterials</category>
      <category>Lloyd-Hughes</category>
      <category>2019</category>
      <pubDate>Sun, 17 Mar 2019 07:40:00 GMT</pubDate>
      <guid isPermaLink="false">8a1785d7697d2d0201698a988ccd4f74</guid>
    </item>
    <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>
    </item>
    <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>
    </item>
    <item>
      <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>
    </item>
    <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>
    </item>
  </channel>
</rss>
