<resource xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns="http://datacite.org/schema/kernel-4" xsi:schemaLocation="http://datacite.org/schema/kernel-4 http://schema.datacite.org/meta/kernel-4.1/metadata.xsd"><identifier identifierType="Handle">21.15109/CONCORDA/YBGOAE</identifier><creators><creator><creatorName nameType="Personal">Himics, László</creatorName><givenName>László</givenName><familyName>Himics</familyName><nameIdentifier nameIdentifierScheme="ORCID">0000-0002-4128-130X</nameIdentifier><affiliation>Wigner Research Centre for Physics</affiliation></creator><creator><creatorName nameType="Personal">Gál, Dávid</creatorName><givenName>Dávid</givenName><familyName>Gál</familyName><nameIdentifier nameIdentifierScheme="ORCID">0000-0002-0661-8544</nameIdentifier><affiliation>Wigner Research Centre for Physics</affiliation></creator><creator><creatorName nameType="Personal">Csíkvári, Péter</creatorName><givenName>Péter</givenName><familyName>Csíkvári</familyName><nameIdentifier nameIdentifierScheme="ORCID">0000-0001-8931-373X</nameIdentifier><affiliation>Budapest University of Technology and Economics</affiliation></creator><creator><creatorName nameType="Personal">Holomb, Roman</creatorName><givenName>Roman</givenName><familyName>Holomb</familyName><nameIdentifier nameIdentifierScheme="ORCID">0000-0002-7383-4183</nameIdentifier><affiliation>Wigner Research Centre for Physics</affiliation></creator><creator><creatorName nameType="Personal">Koós, Margit</creatorName><givenName>Margit</givenName><familyName>Koós</familyName><nameIdentifier nameIdentifierScheme="ScopusID">8417936500</nameIdentifier><affiliation>Wigner Research Centre for Physics</affiliation></creator><creator><creatorName nameType="Personal">Sulyok, Attila</creatorName><givenName>Attila</givenName><familyName>Sulyok</familyName><nameIdentifier nameIdentifierScheme="ScopusID">55974746800</nameIdentifier><affiliation>Centre for Energy Research</affiliation></creator><creator><creatorName nameType="Personal">Pécz, Béla</creatorName><givenName>Béla</givenName><familyName>Pécz</familyName><nameIdentifier nameIdentifierScheme="ORCID">0000-0002-4651-6972</nameIdentifier><affiliation>Centre for Energy Research</affiliation></creator><creator><creatorName nameType="Personal">Veres, Miklós</creatorName><givenName>Miklós</givenName><familyName>Veres</familyName><nameIdentifier nameIdentifierScheme="ORCID">0000-0001-6687-9968</nameIdentifier><affiliation>Wigner Research Centre for Physics</affiliation></creator></creators><titles><title>A modified plasma immersed solid-phase impurity assisted doping geometry for the creation of highly fluorescent CVD nanodiamond</title></titles><publisher>ARP</publisher><publicationYear>2024</publicationYear><subjects><subject>Physics</subject><subject>Fluorescent nanodiamond</subject><subject>Impurity-related color centers</subject><subject>Increased photoluminescence signal</subject><subject>Solid impurity source-assisted doping</subject><subject>Microwave plasma enhanced chemical vapor deposition</subject></subjects><contributors><contributor contributorType="ContactPerson"><contributorName nameType="Personal">Himics, László</contributorName><givenName>László</givenName><familyName>Himics</familyName><affiliation>Wigner Research Centre for Physics</affiliation></contributor></contributors><dates><date dateType="Submitted">2023-11-09</date><date dateType="Updated">2024-04-15</date></dates><resourceType resourceTypeGeneral="Dataset"/><relatedIdentifiers><relatedIdentifier relationType="IsCitedBy" relatedIdentifierType="DOI">10.1016/j.vacuum.2023.112493</relatedIdentifier></relatedIdentifiers><sizes><size>829</size><size>207962</size><size>237694</size><size>2426</size><size>254025</size><size>219939</size><size>32218</size><size>92777</size><size>7736</size><size>586378</size><size>1408762</size><size>5468400</size><size>181892</size><size>10389045</size><size>1465694</size><size>4141666</size><size>331523</size><size>92149</size><size>72140</size><size>132620</size><size>1517056</size></sizes><formats><format>text/plain</format><format>text/plain</format><format>text/plain</format><format>text/plain</format><format>text/plain</format><format>text/plain</format><format>text/plain</format><format>text/plain</format><format>text/plain</format><format>image/tiff</format><format>image/tiff</format><format>image/tiff</format><format>image/tiff</format><format>image/tiff</format><format>image/tiff</format><format>image/tiff</format><format>image/tiff</format><format>image/tiff</format><format>image/tiff</format><format>image/tiff</format><format>application/pdf</format></formats><version>1.0</version><rightsList><rights rightsURI="info:eu-repo/semantics/openAccess"/><rights rightsURI="http://creativecommons.org/licenses/by-nc-nd/4.0">CC BY-NC-ND 4.0</rights></rightsList><descriptions><description descriptionType="Abstract">In this work, we report on a simple and easy to realize doping geometry by which the color center formation efficiency can be improved significantly in nanocrystalline diamond structures during solid impurity source-assisted microwave plasma enhanced chemical vapor deposition (MWCVD). A vertically aligned solid impurity source immersed into the CVD plasma results in diamond thin film with significantly higher color center related fluorescence signal, than the horizontal and source-free arrangements. Based on the example of negatively charged silicon-vacancy (SiV&lt;sup>−&lt;/sup>) center, we demonstrated that the emission peak intensity of fluorescent nanodiamond structures prepared in such a way can be 7–10 times enhanced without significant alteration of the crystal quality. The observed phenomenon is explained by the increased number of incorporated silicon impurities into the diamond nanocrystals, initiated by the beneficial conditions for the atomization of the vertically aligned impurity source, including the enlarged contact area and the elevated surface temperature. The efficiency of the method was demonstrated for thin films and individual nanocrystal structures as well. The proposed solid-phase doping source geometry can be adapted to other impurities to extend the type or improve the in-situ formation efficiency of impurity related color centers in CVD nanodiamond crystals.</description></descriptions><geoLocations/><fundingReferences><fundingReference><funderName>National Research, Development and Innovation Office – NKFI</funderName><awardNumber>OTKA PD-134625</awardNumber></fundingReference><fundingReference><funderName>European Union and European Social Fund</funderName><awardNumber>VEKOP-2.3.2-16-2016-00011</awardNumber></fundingReference><fundingReference><funderName>European Union and European Social Fund</funderName><awardNumber>2018-1.2.1-NKP-2018-00012</awardNumber></fundingReference><fundingReference><funderName>National Research, Development and Innovation Office – NKFI</funderName><awardNumber>2018-1.2.1-NKP</awardNumber></fundingReference></fundingReferences></resource>