<?xml version="1.0" encoding="UTF-8"?><xml><records><record><source-app name="Biblio" version="7.x">Drupal-Biblio</source-app><ref-type>17</ref-type><contributors><authors><author><style face="normal" font="default" size="100%">Pandharkar, Subhash</style></author><author><style face="normal" font="default" size="100%">Rondiya, Sachin</style></author><author><style face="normal" font="default" size="100%">Bhorde, Ajinkya</style></author><author><style face="normal" font="default" size="100%">Nair, Shruthi</style></author><author><style face="normal" font="default" size="100%">Aher, Rahul</style></author><author><style face="normal" font="default" size="100%">Vairale, Priti</style></author><author><style face="normal" font="default" size="100%">Waghmare, Ashish</style></author><author><style face="normal" font="default" size="100%">Naik, Dhirsing</style></author><author><style face="normal" font="default" size="100%">Waykar, Ravindra</style></author><author><style face="normal" font="default" size="100%">Jadhav, Yogesh</style></author></authors></contributors><titles><title><style face="normal" font="default" size="100%">Probing the effect of selenium substitution in kesterite-Cu2ZnSnS4 nanocrystals prepared by hot injection method</style></title><secondary-title><style face="normal" font="default" size="100%">Journal of Materials Science-Materials in Electronics </style></secondary-title></titles><dates><year><style  face="normal" font="default" size="100%">2019</style></year><pub-dates><date><style  face="normal" font="default" size="100%">AUG</style></date></pub-dates></dates><volume><style face="normal" font="default" size="100%">30</style></volume><pages><style face="normal" font="default" size="100%">14781-14790</style></pages><language><style face="normal" font="default" size="100%">eng</style></language><abstract><style face="normal" font="default" size="100%">&lt;p&gt;&lt;span class=&quot;hitHilite&quot;&gt;In&lt;/span&gt; this paper, we report &lt;span class=&quot;hitHilite&quot;&gt;the&lt;/span&gt; &lt;span class=&quot;hitHilite&quot;&gt;effect&lt;/span&gt; &lt;span class=&quot;hitHilite&quot;&gt;of&lt;/span&gt; sulfur (S) &lt;span class=&quot;hitHilite&quot;&gt;substitution&lt;/span&gt; &lt;span class=&quot;hitHilite&quot;&gt;with&lt;/span&gt; &lt;span class=&quot;hitHilite&quot;&gt;selenium&lt;/span&gt; (Se) &lt;span class=&quot;hitHilite&quot;&gt;in&lt;/span&gt; CZTS &lt;span class=&quot;hitHilite&quot;&gt;nanocrystals&lt;/span&gt; &lt;span class=&quot;hitHilite&quot;&gt;prepared&lt;/span&gt; &lt;span class=&quot;hitHilite&quot;&gt;by&lt;/span&gt; &lt;span class=&quot;hitHilite&quot;&gt;hot&lt;/span&gt; &lt;span class=&quot;hitHilite&quot;&gt;injection&lt;/span&gt; &lt;span class=&quot;hitHilite&quot;&gt;method&lt;/span&gt;. &lt;span class=&quot;hitHilite&quot;&gt;The&lt;/span&gt; formation &lt;span class=&quot;hitHilite&quot;&gt;of&lt;/span&gt; kesterite-&lt;span class=&quot;hitHilite&quot;&gt;copper&lt;/span&gt; zinc tin sulfide (Cu2ZnSnS4, CZTS) and &lt;span class=&quot;hitHilite&quot;&gt;copper&lt;/span&gt; zinc tin selenide (Cu2ZnSnSe4, CZTSe) &lt;span class=&quot;hitHilite&quot;&gt;nanocrystals&lt;/span&gt; is confirmed &lt;span class=&quot;hitHilite&quot;&gt;by&lt;/span&gt; X-ray diffraction (XRD), Raman spectroscopy and transmission electron microscopy (TEM) analysis. &lt;span class=&quot;hitHilite&quot;&gt;The&lt;/span&gt; XRD, TEM and atomic force microscopy (AFM) analysis shows an overall increase &lt;span class=&quot;hitHilite&quot;&gt;in&lt;/span&gt; average crystallite size upon Se &lt;span class=&quot;hitHilite&quot;&gt;substitution&lt;/span&gt;. AFM images revealed an increase &lt;span class=&quot;hitHilite&quot;&gt;in&lt;/span&gt; root mean square surface roughness (S-q) and average surface roughness (S-&lt;span class=&quot;hitHilite&quot;&gt;a&lt;/span&gt;) when S &lt;span class=&quot;hitHilite&quot;&gt;in&lt;/span&gt; CZTS is replaced &lt;span class=&quot;hitHilite&quot;&gt;by&lt;/span&gt; Se. &lt;span class=&quot;hitHilite&quot;&gt;The&lt;/span&gt; &lt;span class=&quot;hitHilite&quot;&gt;substitution&lt;/span&gt; &lt;span class=&quot;hitHilite&quot;&gt;of&lt;/span&gt; S &lt;span class=&quot;hitHilite&quot;&gt;by&lt;/span&gt; Se &lt;span class=&quot;hitHilite&quot;&gt;in&lt;/span&gt; host CZTS narrows &lt;span class=&quot;hitHilite&quot;&gt;the&lt;/span&gt; optical band gap from 1.56 to 1.03 eV. &lt;span class=&quot;hitHilite&quot;&gt;The&lt;/span&gt; ultraviolet photoelectron spectroscopy (UPS) analysis shows shift &lt;span class=&quot;hitHilite&quot;&gt;in&lt;/span&gt; valence band and conduction band edge &lt;span class=&quot;hitHilite&quot;&gt;in&lt;/span&gt; CZTSe compared to CZTS. &lt;span class=&quot;hitHilite&quot;&gt;The&lt;/span&gt; photocurrent density measurement &lt;span class=&quot;hitHilite&quot;&gt;in&lt;/span&gt; synthesized CZTSe thin films is similar to 4 to 5 times higher than CZTS thin films. &lt;span class=&quot;hitHilite&quot;&gt;The&lt;/span&gt; obtained results show that CZTSe can be &lt;span class=&quot;hitHilite&quot;&gt;a&lt;/span&gt; promising candidate as absorber material &lt;span class=&quot;hitHilite&quot;&gt;in&lt;/span&gt; photovoltaic applications.&lt;/p&gt;
</style></abstract><issue><style face="normal" font="default" size="100%">15</style></issue><work-type><style face="normal" font="default" size="100%">Article</style></work-type><custom3><style face="normal" font="default" size="100%">&lt;p&gt;Foreign&lt;/p&gt;
</style></custom3><custom4><style face="normal" font="default" size="100%">&lt;p&gt;&lt;span&gt;2.195&lt;/span&gt;&lt;/p&gt;
</style></custom4></record><record><source-app name="Biblio" version="7.x">Drupal-Biblio</source-app><ref-type>17</ref-type><contributors><authors><author><style face="normal" font="default" size="100%">Rahane, Swati N.</style></author><author><style face="normal" font="default" size="100%">Rahane, Ganesh K.</style></author><author><style face="normal" font="default" size="100%">Mandal, Animesh</style></author><author><style face="normal" font="default" size="100%">Jadhav, Yogesh</style></author><author><style face="normal" font="default" size="100%">Godha, Akshat</style></author><author><style face="normal" font="default" size="100%">Rokade, Avinash</style></author><author><style face="normal" font="default" size="100%">Shah, Shruti</style></author><author><style face="normal" font="default" size="100%">Hase, Yogesh</style></author><author><style face="normal" font="default" size="100%">Waghmare, Ashish</style></author><author><style face="normal" font="default" size="100%">Saykar, Nilesh G.</style></author><author><style face="normal" font="default" size="100%">Roy, Anurag</style></author><author><style face="normal" font="default" size="100%">Salgaonkar, Kranti N.</style></author><author><style face="normal" font="default" size="100%">Dubal, Deepak</style></author><author><style face="normal" font="default" size="100%">Makineni, Surendra K.</style></author><author><style face="normal" font="default" size="100%">Dzade, Nelson Y.</style></author><author><style face="normal" font="default" size="100%">Jadkar, Sandesh R.</style></author><author><style face="normal" font="default" size="100%">Rondiya, Sachin R.</style></author></authors></contributors><titles><title><style face="normal" font="default" size="100%">Lead-free Cs2AgBiCl6 double perovskite: experimental and theoretical insights into the self-trapping for optoelectronic applications</style></title><secondary-title><style face="normal" font="default" size="100%">ACS Physical Chemistry Au</style></secondary-title></titles><dates><year><style  face="normal" font="default" size="100%">2024</style></year><pub-dates><date><style  face="normal" font="default" size="100%">JUL</style></date></pub-dates></dates><volume><style face="normal" font="default" size="100%">4</style></volume><pages><style face="normal" font="default" size="100%">476–489</style></pages><language><style face="normal" font="default" size="100%">eng</style></language><abstract><style face="normal" font="default" size="100%">&lt;p&gt;
	&lt;span style=&quot;color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif; font-size: 16px;&quot;&gt;Lead-free double perovskites (DPs) will emerge as viable and environmentally safe substitutes for Pb-halide perovskites, demonstrating stability and nontoxicity if their optoelectronic property is greatly improved. Doping has been experimentally validated as a powerful tool for enhancing optoelectronic properties and concurrently reducing the defect state density in DP materials. Fundamental understanding of the optical properties of DPs, particularly the self-trapped exciton (STEs) dynamics, plays a critical role in a range of optoelectronic applications. Our study investigates how Fe doping influences the structural and optical properties of Cs&lt;/span&gt;&lt;span style=&quot;box-sizing: border-box; outline: none; line-height: 0; position: relative; vertical-align: baseline; bottom: -0.25em; color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif;&quot;&gt;2&lt;/span&gt;&lt;span style=&quot;color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif; font-size: 16px;&quot;&gt;AgBiCl&lt;/span&gt;&lt;span style=&quot;box-sizing: border-box; outline: none; line-height: 0; position: relative; vertical-align: baseline; bottom: -0.25em; color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif;&quot;&gt;6&lt;/span&gt;&lt;span style=&quot;color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif; font-size: 16px;&quot;&gt;&amp;nbsp;DPs by understanding their STEs dynamics, which is currently lacking in the literature. A combined experimental–computational approach is employed to investigate the optoelectronic properties of pure and doped Cs&lt;/span&gt;&lt;span style=&quot;box-sizing: border-box; outline: none; line-height: 0; position: relative; vertical-align: baseline; bottom: -0.25em; color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif;&quot;&gt;2&lt;/span&gt;&lt;span style=&quot;color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif; font-size: 16px;&quot;&gt;AgBiCl&lt;/span&gt;&lt;span style=&quot;box-sizing: border-box; outline: none; line-height: 0; position: relative; vertical-align: baseline; bottom: -0.25em; color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif;&quot;&gt;6&lt;/span&gt;&lt;span style=&quot;color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif; font-size: 16px;&quot;&gt;&amp;nbsp;(Fe–Cs&lt;/span&gt;&lt;span style=&quot;box-sizing: border-box; outline: none; line-height: 0; position: relative; vertical-align: baseline; bottom: -0.25em; color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif;&quot;&gt;2&lt;/span&gt;&lt;span style=&quot;color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif; font-size: 16px;&quot;&gt;AgBiCl&lt;/span&gt;&lt;span style=&quot;box-sizing: border-box; outline: none; line-height: 0; position: relative; vertical-align: baseline; bottom: -0.25em; color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif;&quot;&gt;6&lt;/span&gt;&lt;span style=&quot;color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif; font-size: 16px;&quot;&gt;) perovskites. Successful incorporation of Fe&lt;/span&gt;&lt;span style=&quot;box-sizing: border-box; outline: none; line-height: 0; position: relative; vertical-align: baseline; top: -0.5em; color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif;&quot;&gt;3+&lt;/span&gt;&lt;span style=&quot;color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif; font-size: 16px;&quot;&gt;&amp;nbsp;ions is confirmed by X-ray diffraction and Raman spectroscopy. Moreover, the Fe–Cs&lt;/span&gt;&lt;span style=&quot;box-sizing: border-box; outline: none; line-height: 0; position: relative; vertical-align: baseline; bottom: -0.25em; color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif;&quot;&gt;2&lt;/span&gt;&lt;span style=&quot;color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif; font-size: 16px;&quot;&gt;AgBiCl&lt;/span&gt;&lt;span style=&quot;box-sizing: border-box; outline: none; line-height: 0; position: relative; vertical-align: baseline; bottom: -0.25em; color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif;&quot;&gt;6&lt;/span&gt;&lt;span style=&quot;color: rgb(21, 21, 21); font-family: Roboto, arial, sans-serif; font-size: 16px;&quot;&gt;&amp;nbsp;DPs exhibit strong absorption from below 400 nm up to 700 nm, indicating sub-band gap state transitions originating from surface defects. Photoluminescence (PL) analysis demonstrates a significant enhancement in the PL intensity, attributed to an increased radiative recombination rate and higher STE density. The radiative kinetics and average lifetime are investigated by the time-resolved PL (TRPL) method; in addition, temperature-dependent PL measurements provide valuable insights into activation energy and exciton–phonon coupling strength. Our findings will not only deepen our understanding of charge carrier dynamics associated with STEs but also pave the way for the design of some promising perovskite materials for use in optoelectronics and photocatalysis.&lt;/span&gt;&lt;/p&gt;
</style></abstract><issue><style face="normal" font="default" size="100%">5</style></issue><work-type><style face="normal" font="default" size="100%">Article</style></work-type><custom3><style face="normal" font="default" size="100%">&lt;p&gt;
	Foreign&lt;/p&gt;
</style></custom3><custom4><style face="normal" font="default" size="100%">&lt;p&gt;
	3.7&lt;/p&gt;
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