<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Malik Z</submitter><funding>European Research Council</funding><funding>Engineering and Physical Sciences Research Council</funding><pagination>17574-17586</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC11440232</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>12(43)</volume><pubmed_abstract>The optoelectronic properties of two layered copper oxyselenide compounds, with nominal composition Sr&lt;sub>2&lt;/sub>ZnO&lt;sub>2&lt;/sub>Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub> and Ba&lt;sub>2&lt;/sub>ZnO&lt;sub>2&lt;/sub>Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub>, have been investigated to determine their suitability as p-type conductors. The structure, band gaps and electrical conductivity of pristine and alkali-metal-doped samples have been determined. We find that the strontium-containing compound, Sr&lt;sub>2&lt;/sub>ZnO&lt;sub>2&lt;/sub>Cu&lt;sub>2&lt;/sub>Se&lt;sub&gt;2&lt;/sub>, adopts the expected tetragonal &lt;i>Sr&lt;/i> &lt;sub>&lt;i>2&lt;/i>&lt;/sub> &lt;i>Mn&lt;/i> &lt;sub>&lt;i>3&lt;/i>&lt;/sub> &lt;i>SbO&lt;/i> &lt;sub>&lt;i>2&lt;/i>&lt;/sub> structure with &lt;i>I&lt;/i>4/&lt;i>mmm&lt;/i> symmetry, and has a band gap of 2.16 eV, and a room temperature conductivity of 4.8 × 10&lt;sup>-1&lt;/sup> S cm&lt;sup>-1&lt;/sup>. The conductivity of the compound could be increased to 4.2 S cm&lt;sup>-1&lt;/sup> when sodium doped to a nominal composition of Na&lt;sub>0.1&lt;/sub>Sr&lt;sub>1.9&lt;/sub>ZnO&lt;sub>2&lt;/sub>Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub>. In contrast, the barium containing material was found to have a small zinc oxide deficiency, with a sample dependent compositional range of Ba&lt;sub>2&lt;/sub>Zn&lt;sub>1-&lt;i>x&lt;/i>&lt;/sub> O&lt;sub>2-&lt;i>x&lt;/i>&lt;/sub> Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub> where 0.01 &lt; &lt;i>x&lt;/i> &lt; 0.06, as determined by single crystal X-ray diffraction and powder neutron diffraction. The barium-containing structure could also be modelled using the tetragonal &lt;i>I&lt;/i>4/&lt;i>mmm&lt;/i> structure, but significant elongation of the oxygen displacement ellipsoid along the Zn-O bonds in the average structure was observed. This indicated that the oxide ion position was better modelled as a disordered split site with a displacement to change the local zinc coordination from square planar to linear. Electron diffraction data confirmed that the oxide site in Ba&lt;sub>2&lt;/sub>Zn&lt;sub>1-&lt;i>x&lt;/i>&lt;/sub> O&lt;sub>2-&lt;i>x&lt;/i>&lt;/sub> Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub> does not adopt a long range ordered arrangement, but also that the idealised &lt;i>I&lt;/i>4/&lt;i>mmm&lt;/i> structure with an unsplit oxide site was not consistent with the extra reflections observed in the electron diffractograms. The band gap and conductivity of Ba&lt;sub>2&lt;/sub>Zn&lt;sub>1-&lt;i>x&lt;/i>&lt;/sub> O&lt;sub>2-&lt;i>x&lt;/i>&lt;/sub> Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub> were determined to be 2.22 eV and 2.0 × 10&lt;sup>-3&lt;/sup> S cm&lt;sup>-1&lt;/sup> respectively. The conductivity could be increased to 1.5 × 10&lt;sup>-1&lt;/sup> S cm&lt;sup>-1&lt;/sup> with potassium doping in K&lt;sub>0.1&lt;/sub>Ba&lt;sub>1.9&lt;/sub>Zn&lt;sub>1-&lt;i>x&lt;/i>&lt;/sub> O&lt;sub>2-&lt;i>x&lt;/i>&lt;/sub> Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub>. Hall measurements confirmed that both materials were p-type conductors with holes as the dominant charge carriers.</pubmed_abstract><journal>Journal of materials chemistry. C</journal><pubmed_title>Observation and enhancement through alkali metal doping of p-type conductivity in the layered oxyselenides Sr&lt;sub>2&lt;/sub>ZnO&lt;sub>2&lt;/sub>Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub> and Ba&lt;sub>2&lt;/sub>Zn&lt;sub>1-&lt;i>x&lt;/i>&lt;/sub> O&lt;sub>2-&lt;i>x&lt;/i>&lt;/sub> Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub>.</pubmed_title><pmcid>PMC11440232</pmcid><funding_grant_id>EP/W032244/1</funding_grant_id><funding_grant_id>EP/P020194/1</funding_grant_id><funding_grant_id>EP/T011793/1</funding_grant_id><funding_grant_id>EP/R029431</funding_grant_id><funding_grant_id>758345</funding_grant_id><funding_grant_id>EP/T022213/1</funding_grant_id><funding_grant_id>EP/W032260/1</funding_grant_id><funding_grant_id>EP/T027991/1</funding_grant_id><funding_grant_id>EP/L000202</funding_grant_id><funding_grant_id>EP/T022108/1</funding_grant_id><pubmed_authors>Gal ZA</pubmed_authors><pubmed_authors>Smyth RD</pubmed_authors><pubmed_authors>Huang R</pubmed_authors><pubmed_authors>Newbrook DW</pubmed_authors><pubmed_authors>Kemp L</pubmed_authors><pubmed_authors>Blandy JN</pubmed_authors><pubmed_authors>Herkelrath SJC</pubmed_authors><pubmed_authors>Davies DW</pubmed_authors><pubmed_authors>Hyett G</pubmed_authors><pubmed_authors>Broadley S</pubmed_authors><pubmed_authors>Clarke SJ</pubmed_authors><pubmed_authors>Malik Z</pubmed_authors><pubmed_authors>Scanlon DO</pubmed_authors><pubmed_authors>Rutt G</pubmed_authors><pubmed_authors>Hadermann J</pubmed_authors></additional><is_claimable>false</is_claimable><name>Observation and enhancement through alkali metal doping of p-type conductivity in the layered oxyselenides Sr&lt;sub>2&lt;/sub>ZnO&lt;sub>2&lt;/sub>Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub> and Ba&lt;sub>2&lt;/sub>Zn&lt;sub>1-&lt;i>x&lt;/i>&lt;/sub> O&lt;sub>2-&lt;i>x&lt;/i>&lt;/sub> Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub>.</name><description>The optoelectronic properties of two layered copper oxyselenide compounds, with nominal composition Sr&lt;sub>2&lt;/sub>ZnO&lt;sub>2&lt;/sub>Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub> and Ba&lt;sub>2&lt;/sub>ZnO&lt;sub>2&lt;/sub>Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub>, have been investigated to determine their suitability as p-type conductors. The structure, band gaps and electrical conductivity of pristine and alkali-metal-doped samples have been determined. We find that the strontium-containing compound, Sr&lt;sub>2&lt;/sub>ZnO&lt;sub>2&lt;/sub>Cu&lt;sub>2&lt;/sub>Se&lt;sub&gt;2&lt;/sub>, adopts the expected tetragonal &lt;i>Sr&lt;/i> &lt;sub>&lt;i>2&lt;/i>&lt;/sub> &lt;i>Mn&lt;/i> &lt;sub>&lt;i>3&lt;/i>&lt;/sub> &lt;i>SbO&lt;/i> &lt;sub>&lt;i>2&lt;/i>&lt;/sub> structure with &lt;i>I&lt;/i>4/&lt;i>mmm&lt;/i> symmetry, and has a band gap of 2.16 eV, and a room temperature conductivity of 4.8 × 10&lt;sup>-1&lt;/sup> S cm&lt;sup>-1&lt;/sup>. The conductivity of the compound could be increased to 4.2 S cm&lt;sup>-1&lt;/sup> when sodium doped to a nominal composition of Na&lt;sub>0.1&lt;/sub>Sr&lt;sub>1.9&lt;/sub>ZnO&lt;sub>2&lt;/sub>Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub>. In contrast, the barium containing material was found to have a small zinc oxide deficiency, with a sample dependent compositional range of Ba&lt;sub>2&lt;/sub>Zn&lt;sub>1-&lt;i>x&lt;/i>&lt;/sub> O&lt;sub>2-&lt;i>x&lt;/i>&lt;/sub> Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub> where 0.01 &lt; &lt;i>x&lt;/i> &lt; 0.06, as determined by single crystal X-ray diffraction and powder neutron diffraction. The barium-containing structure could also be modelled using the tetragonal &lt;i>I&lt;/i>4/&lt;i>mmm&lt;/i> structure, but significant elongation of the oxygen displacement ellipsoid along the Zn-O bonds in the average structure was observed. This indicated that the oxide ion position was better modelled as a disordered split site with a displacement to change the local zinc coordination from square planar to linear. Electron diffraction data confirmed that the oxide site in Ba&lt;sub>2&lt;/sub>Zn&lt;sub>1-&lt;i>x&lt;/i>&lt;/sub> O&lt;sub>2-&lt;i>x&lt;/i>&lt;/sub> Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub> does not adopt a long range ordered arrangement, but also that the idealised &lt;i>I&lt;/i>4/&lt;i>mmm&lt;/i> structure with an unsplit oxide site was not consistent with the extra reflections observed in the electron diffractograms. The band gap and conductivity of Ba&lt;sub>2&lt;/sub>Zn&lt;sub>1-&lt;i>x&lt;/i>&lt;/sub> O&lt;sub>2-&lt;i>x&lt;/i>&lt;/sub> Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub> were determined to be 2.22 eV and 2.0 × 10&lt;sup>-3&lt;/sup> S cm&lt;sup>-1&lt;/sup> respectively. The conductivity could be increased to 1.5 × 10&lt;sup>-1&lt;/sup> S cm&lt;sup>-1&lt;/sup> with potassium doping in K&lt;sub>0.1&lt;/sub>Ba&lt;sub>1.9&lt;/sub>Zn&lt;sub>1-&lt;i>x&lt;/i>&lt;/sub> O&lt;sub>2-&lt;i>x&lt;/i>&lt;/sub> Cu&lt;sub>2&lt;/sub>Se&lt;sub>2&lt;/sub>. Hall measurements confirmed that both materials were p-type conductors with holes as the dominant charge carriers.</description><dates><release>2024-01-01T00:00:00Z</release><publication>2024 Nov</publication><modification>2026-05-29T09:31:57.177Z</modification><creation>2025-04-04T22:47:51.55Z</creation></dates><accession>S-EPMC11440232</accession><cross_references><pubmed>39360290</pubmed><doi>10.1039/d4tc02458c</doi></cross_references></HashMap>