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Numerical design and analysis of bilayer absorber perovskite solar cells based on Cs2TiF6 and CsSnI3 基于Cs2TiF6和CsSnI3的双层吸收钙钛矿太阳能电池的数值设计与分析
IF 4.9 3区 材料科学 Q2 CHEMISTRY, MULTIDISCIPLINARY Pub Date : 2025-12-25 DOI: 10.1016/j.jpcs.2025.113494
Siham Mansouri , Kamal Zeghdar , Lakhdar Dehimi , Fortunato Pezzimenti , Ripel Chakma , Abdullah M.S. Alhuthali , Alsharef Mohammad , Ayman A. Aly , Nacer Badi , Mohamed H.H. Mahmoud , Rajesh Haldhar , M. Khalid Hossain
Lead-free all-inorganic perovskites have emerged as promising materials for environmentally sustainable photovoltaic technologies. In this study, SCAPS-1D simulations are employed to investigate the optoelectronic behavior of Cs2TiF6 and CsSnI3 absorbers in both single-layer and bilayer device configurations. By systematically varying absorber thickness, acceptor doping concentration, and bulk defect density, the work establishes how these intrinsic material parameters influence charge generation, recombination dynamics, and overall device performance. The simulations show that Cs2TiF6-based devices exhibit high open-circuit voltage due to their wide bandgap, while CsSnI3 enables strong current generation stemming from its narrow bandgap and efficient near-infrared absorption. Integrating the two materials into a bilayer absorber architecture combines these advantages, enhancing spectral utilization and promoting more effective charge separation across the internal interface. Under idealized low-defect conditions, the bilayer device reaches a maximum theoretical efficiency of 32.93 %, whereas realistic defect densities typical of solution-processed Cs-based perovskites (1015-1018 cm−3) yield efficiencies in the range of 12–26 %. The study further highlights the sensitivity of device behavior to defect concentration, doping levels, and absorber–absorber interface quality, and it clarifies how these factors shape the operational limits of lead-free perovskite solar cells. By mapping the relationships between absorber properties and photovoltaic response, the work outlines design principles that can support the development of scalable, stable, and high-performance lead-free perovskite photovoltaics.
无铅全无机钙钛矿已成为环境可持续光伏技术的有前途的材料。在本研究中,采用SCAPS-1D模拟研究了Cs2TiF6和CsSnI3在单层和双层器件配置下的光电行为。通过系统地改变吸收体厚度、受体掺杂浓度和体缺陷密度,该工作建立了这些固有材料参数如何影响电荷产生、重组动力学和整体器件性能。仿真结果表明,基于cs2tif6的器件由于其宽带隙而具有高开路电压,而基于CsSnI3的器件由于其窄带隙和高效的近红外吸收而具有强电流产生。将这两种材料集成到双层吸收结构中,结合了这些优点,提高了光谱利用率,并促进了内部界面上更有效的电荷分离。在理想的低缺陷条件下,双层器件的最大理论效率达到32.93%,而实际缺陷密度典型的溶液处理cs基钙钛矿(1015-1018 cm−3)的产率在12 - 26%之间。该研究进一步强调了器件行为对缺陷浓度、掺杂水平和吸收-吸收界面质量的敏感性,并阐明了这些因素如何影响无铅钙钛矿太阳能电池的工作极限。通过绘制吸收剂特性和光伏响应之间的关系,该工作概述了可以支持可扩展、稳定和高性能无铅钙钛矿光伏电池开发的设计原则。
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引用次数: 0
Development of a magnetic bifunctional catalyst based on modified carbon quantum dots for CO2 fixation under solvent- and cocatalyst-free conditions 基于改性碳量子点的磁性双功能催化剂在无溶剂和无助催化剂条件下固定CO2的研究
IF 4.9 3区 材料科学 Q2 CHEMISTRY, MULTIDISCIPLINARY Pub Date : 2025-12-24 DOI: 10.1016/j.jpcs.2025.113481
Saeed Torabi, Golnoosh Ghafari Tirabadi, Mohammad Taghi Nazeri, Ahmad Shaabani
The synergistic effect of multiple active centers is an efficient strategy for intelligent control in catalysis. However, the challenge lies in the simultaneous and organized integration of various active species into a porous support. Among the various classes of multifunctional catalysts, those containing both Lewis acid (LA) and Lewis base (LB) sites, which can facilitate cocatalyst-free cycloaddition of CO2 with epoxides, have garnered significant attention. This study utilized carbon quantum dots (CQDs) as an efficient and environmentally friendly support to develop a magnetic bifunctional catalyst through a targeted approach. Specifically, pre-magnetized CQDs nanoparticles (CQDs@Fe3O4) were involved in the Betti three-component reaction (Betti-3CR) of pyridine-4-carbaldehyde and β-naphthol to introduce α-aminophenol functional groups onto CQDs as ligands. LA and LB sites were readily generated on the Betti-CQDs@Fe3O4 using cobalt salt and ethyl bromide, respectively. The resulting Co(II)@Betti-CQDs@Fe3O4 bromide was characterized through various analyses, including FT-IR, VSM, XRD, TEM, SEM, EDAX-EDS, TGA, BET, and ICP-OES. The effectiveness of Co(II)@Betti-CQDs@Fe3O4 bromide as a heterogeneous bifunctional catalyst was investigated in the CO2 fixation reaction under solvent- and cocatalyst-free conditions. The results demonstrated that the desired products were synthesized rapidly with high yields. The favorable catalytic performance arises from the efficient CO2 adsorption capacity of the CQDs as a magnetized support, combined with the synergistic effect of the LA and LB active centers in the bifunctional catalyst. Furthermore, this appealing catalyst is user-friendly, exhibits minimal leaching of cobalt into the reaction medium, displays significant CO2 absorption capacity, and is readily reusable.
多活性中心协同作用是实现催化智能控制的有效策略。然而,挑战在于将各种活性物种同时有组织地整合到多孔支撑中。在各种类型的多功能催化剂中,同时含有路易斯酸(LA)和路易斯碱(LB)位点的催化剂能够促进二氧化碳与环氧化物的无共催化剂环加成,引起了人们的广泛关注。本研究利用碳量子点(CQDs)作为一种高效环保的载体,通过有针对性的方法开发了磁性双功能催化剂。具体来说,预磁化CQDs纳米粒子(CQDs@Fe3O4)参与了吡啶-4-醛和β-萘酚的Betti三组分反应(Betti- 3cr),将α-氨基酚官能团作为配体引入CQDs上。在Betti-CQDs@Fe3O4上分别用钴盐和溴乙基制备了LA和LB位点。通过FT-IR、VSM、XRD、TEM、SEM、EDAX-EDS、TGA、BET和ICP-OES等多种分析手段对Co(II)@Betti-CQDs@Fe3O4溴化物进行了表征。研究了Co(II)@Betti-CQDs@Fe3O4溴化物在无溶剂和无助催化剂条件下作为非均相双功能催化剂在CO2固定反应中的效果。结果表明,合成所需产物速度快,收率高。由于CQDs作为磁化载体具有高效的CO2吸附能力,再加上双功能催化剂中LA和LB活性中心的协同作用,使得CQDs具有良好的催化性能。此外,这种吸引人的催化剂是用户友好的,表现出最少的钴浸出到反应介质中,表现出显著的二氧化碳吸收能力,并且易于重复使用。
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引用次数: 0
A comprehensive review of phosphate-based acid geopolymers: production, properties, and applications 综述了磷酸基酸性地聚合物的生产、性能和应用
IF 4.9 3区 材料科学 Q2 CHEMISTRY, MULTIDISCIPLINARY Pub Date : 2025-12-23 DOI: 10.1016/j.jpcs.2025.113489
Gabriel Tochetto , Karine Goulart Oliveira , Marco D'Agostini , Giorgia Franchin , Hamada Elsayed , Dachamir Hotza , Maria Eliza Nagel-Hassemer , Paolo Colombo
Phosphate-based geopolymers have emerged as versatile and sustainable materials with distinct advantages over traditional binders. Formed through acid-based activation, typically using phosphoric acid, these geopolymers exhibit unique features such as enhanced chemical resistance, tunable porosity, and compatibility with a wide range of raw materials, including industrial residues. This review provides a comprehensive overview of the synthesis mechanisms, structural evolution, and functional properties of phosphate-based geopolymers. Particular emphasis is placed on their applications in waste stabilization, soil remediation, and adsorption and catalytic processes for environmental management. Additionally, this study discusses current challenges and future research directions, including the optimization of synthesis parameters, the incorporation of additives such as laponite, bentonite, and silica to improve rheology and mechanical strength, and the development of hybrid systems that combine inorganic and organic components to tailor performance. By integrating recent findings, this review underscores the potential of phosphate-based geopolymers as next-generation materials for sustainable engineering and environmental remediation. This review adopts a process-structure-property-application framework to explain how precursor selection, mix design, and curing conditions govern the viability of phosphate geopolymers across targeted environmental and high-temperature applications, including emerging extrusion-based additive manufacturing.
磷酸盐基地聚合物已成为一种多功能和可持续的材料,与传统粘合剂相比具有明显的优势。这些地聚合物通过酸基活化形成,通常使用磷酸,具有独特的特性,如增强的耐化学性,可调节的孔隙率,以及与各种原材料(包括工业残留物)的相容性。本文综述了磷酸盐基地聚合物的合成机理、结构演变和功能特性。特别强调它们在废物稳定,土壤修复以及环境管理的吸附和催化过程中的应用。此外,本研究还讨论了当前面临的挑战和未来的研究方向,包括优化合成参数,加入拉脱土、膨润土和二氧化硅等添加剂以改善流变性和机械强度,以及开发结合无机和有机成分的混合体系以定制性能。通过整合最近的研究成果,本综述强调了磷酸盐基地聚合物作为可持续工程和环境修复的下一代材料的潜力。本文采用工艺-结构-性能-应用框架来解释前驱体选择、混合设计和固化条件如何影响磷酸盐地聚合物在目标环境和高温应用中的可行性,包括新兴的基于挤压的增材制造。
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引用次数: 0
Nature and trend of defect doping in Ca3N2: A first-principles investigation Ca3N2中缺陷掺杂的性质和趋势:第一性原理研究
IF 4.9 3区 材料科学 Q2 CHEMISTRY, MULTIDISCIPLINARY Pub Date : 2025-12-23 DOI: 10.1016/j.jpcs.2025.113486
Shouze Qiu, Peng Xu, Liyin Zhang, Shun Guo, Jingya Tang
The asymmetry in defect doping behavior has been widely observed across various nitride materials. In this study, we report a significant doping asymmetry in α-Ca3N2: p-type doping is strongly inhibited, whereas n-type doping is comparatively achievable, with lighter elements demonstrating greater effectiveness as dopants than their heavier counterparts. Using hybrid functional calculations in conjunction with self-consistent Fermi level analysis, we conduct a comprehensive first-principles investigation into the defect physics and doping characteristics of the wide-bandgap alkaline-earth nitride α-Ca3N2. Our findings indicate that intrinsic defects inherently favor n-type conductivity in α-Ca3N2, while p-type doping faces substantial challenges. These limitations arise primarily from the prevalence of nitrogen vacancies, the scarcity of dopants that simultaneously possess high solubility and shallow acceptor levels, and the relatively low valence band maximum (VBM) of Ca3N2. For n-type doping, elements including H, Si, Ge, Ga, O, and S are identified as viable candidates, with interstitial Si and Ge exhibiting particularly high doping efficiencies, whereas other dopants show limited efficacy. This observed doping trend not only extends to other group-II nitrides but also offers valuable guidance for the development of wide-bandgap nitride semiconductors more broadly.
在各种氮化物材料中,缺陷掺杂行为的不对称性已被广泛观察到。在这项研究中,我们报道了α-Ca3N2中明显的掺杂不对称性:p型掺杂被强烈抑制,而n型掺杂相对来说是可以实现的,较轻的元素比较重的元素表现出更大的掺杂效果。利用杂化泛函计算结合自相容费米能级分析,对宽禁带碱土氮化物α-Ca3N2的缺陷物理和掺杂特性进行了全面的第一性原理研究。我们的研究结果表明,α-Ca3N2中固有缺陷有利于n型电导率,而p型掺杂面临着巨大的挑战。这些限制主要来自于氮空位的普遍存在,同时具有高溶解度和浅受体水平的掺杂物的稀缺性,以及Ca3N2相对较低的价带最大值(VBM)。对于n型掺杂,包括H、Si、Ge、Ga、O和S在内的元素被确定为可行的候选元素,其中Si和Ge具有特别高的掺杂效率,而其他掺杂剂的效率有限。这种观察到的掺杂趋势不仅延伸到其他ii族氮化物,而且为更广泛地发展宽带隙氮化物半导体提供了有价值的指导。
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引用次数: 0
Time-resolved microwave conductivity of P25 TiO2: Distinguishing light-induced electron and hole transport P25 TiO2的时间分辨微波电导率:区分光致电子和空穴输运
IF 4.9 3区 材料科学 Q2 CHEMISTRY, MULTIDISCIPLINARY Pub Date : 2025-12-23 DOI: 10.1016/j.jpcs.2025.113488
C. Colbeau-Justin , A. Kanaev
Time-resolved microwave conductivity measurements were carried out on P25 TiO2 powder, dry and wetted with ethanol and water, at room temperature with pulsed laser excitation at 360 nm. Using a power-law model, major channels of the charge relaxation kinetics were distinguished and identified. These are related to recombination of (1) electrons with holes trapped on shallow bulk defects and (2) electrons released from surface/bulk states with deeply trapped holes. The shallow bulk traps form a reservoir of energy in equilibrium with the continuous band states preserving the plasma-like charges recombination during ∼200 ns after the excitation. On a longer μs-ms timescale the recombination slows down because of the deep hole traps population, matching the power law kinetics.
在室温下,在360 nm脉冲激光激发下,对P25 TiO2粉末进行时间分辨微波电导率的测量。利用幂律模型,对电荷弛豫动力学的主要通道进行了区分和识别。这与(1)在浅体缺陷上捕获空穴的电子和(2)从表面/体状态释放的具有深捕获空穴的电子的复合有关。在激发后的~ 200ns内,浅体阱形成了一个能量平衡库,连续带态保持了类等离子体电荷的复合。在较长的μs-ms时间尺度上,由于深孔阱的数量,复合速度减慢,符合幂律动力学。
{"title":"Time-resolved microwave conductivity of P25 TiO2: Distinguishing light-induced electron and hole transport","authors":"C. Colbeau-Justin ,&nbsp;A. Kanaev","doi":"10.1016/j.jpcs.2025.113488","DOIUrl":"10.1016/j.jpcs.2025.113488","url":null,"abstract":"<div><div>Time-resolved microwave conductivity measurements were carried out on P25 TiO<sub>2</sub> powder, dry and wetted with ethanol and water, at room temperature with pulsed laser excitation at 360 nm. Using a power-law model, major channels of the charge relaxation kinetics were distinguished and identified. These are related to recombination of (1) electrons with holes trapped on shallow bulk defects and (2) electrons released from surface/bulk states with deeply trapped holes. The shallow bulk traps form a reservoir of energy in equilibrium with the continuous band states preserving the plasma-like charges recombination during ∼200 ns after the excitation. On a longer μs-ms timescale the recombination slows down because of the deep hole traps population, matching the power law kinetics.</div></div>","PeriodicalId":16811,"journal":{"name":"Journal of Physics and Chemistry of Solids","volume":"211 ","pages":"Article 113488"},"PeriodicalIF":4.9,"publicationDate":"2025-12-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145837419","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Structural, microstructural, impedance spectroscopy and dielectric studies on La2Co1-xZnxMnO6 (x=0, 0.05 and 0.1) double perovskite La2Co1-xZnxMnO6 (x= 0,0.05和0.1)双钙钛矿的结构、微观结构、阻抗谱和介电特性研究
IF 4.9 3区 材料科学 Q2 CHEMISTRY, MULTIDISCIPLINARY Pub Date : 2025-12-23 DOI: 10.1016/j.jpcs.2025.113497
Swagatika Mohanty , A.K. Biswal , J. Ray
<div><div>La<sub>2</sub>Co<sub>1-x</sub>Zn<sub>x</sub>MnO<sub>6</sub> (x = 0, 0.05 and 0.1) samples were synthesized via the sol–gel auto-combustion method and systematically characterized. Rietveld refinement of room-temperature X-ray diffraction confirmed a single-phase monoclinic structure (space group <em>P2</em><sub><em>1</em></sub><em>/n</em>), with negligible change in lattice parameters at 5 % Zn substitution but a pronounced expansion at 10 %. Analysis of FESEM images revealed the increase in average grain sizes: 112 ± 35 nm (x = 0), 121 ± 36 nm (x = 0.05) and 187 ± 66 nm (x = 0.1), with reduced porosity:15.3 % (x = 0), 14 % (x = 0.05) and 5.74 % (x = 0.1) upon Zn doping. Impedance spectra analysed using the Havriliak–Negami model yielded resistance (R), relaxation time (<span><math><msub><mi>τ</mi><mi>Z</mi></msub></math></span>), asymmetry (α), and broadness (β) parameters, showing a significant rise in R and <span><math><mrow><msub><mi>τ</mi><mi>z</mi></msub></mrow></math></span> for the 10 % doped sample across all temperatures. A.C. electrical transport examined from temperature dependent ‘R’ followed variable-range hopping (VRH), with Mott temperatures (<span><math><mrow><msub><mi>T</mi><mn>0</mn></msub></mrow></math></span>) of 1.186 × 10<sup>9</sup> K, 1.54 × 10<sup>9</sup> K, and 6.568 × 10<sup>9</sup> K for x = 0, 0.05, and 0.1, respectively. Density of states of the charge carriers at the Fermi level are <span><math><mrow><mn>2.34</mn><mo>×</mo><msup><mn>10</mn><mn>19</mn></msup></mrow></math></span> ev<sup>−1</sup>.cm<sup>−3</sup> for x = 0, <span><math><mrow><mn>1.83</mn><mo>×</mo><msup><mn>10</mn><mn>19</mn></msup></mrow></math></span> ev<sup>−1</sup>.cm<sup>−3</sup> for x = 0.05 and <span><math><mrow><mn>3.60</mn><mo>×</mo><msup><mn>10</mn><mn>18</mn></msup></mrow></math></span> ev<sup>−1</sup>.cm<sup>−3</sup> for x = 0.1. A conduction crossover pertaining to trapped state of shallow donors was observed in the 10 % doped sample between temperature range 303 K–363 K with activation energy 0.049 eV <span><math><mrow><msub><mi>τ</mi><mi>z</mi></msub></mrow></math></span> shows thermally activated behaviour with Activation energy (<span><math><mrow><msub><mi>E</mi><mi>a</mi></msub></mrow></math></span>) values 0.33 eV (x = 0), 0.35 eV (x = 0.05) and 0.53 eV (x = 0.1). Shallow trap state is also seen in temperature dependent <span><math><mrow><msub><mi>τ</mi><mi>z</mi></msub></mrow></math></span> for x = 0.1 has value 0.041 eV. Modulus spectra fitted with the Kohlrausch–Williams–Watts function calculated ‘<span><math><mrow><msub><mi>τ</mi><mi>m</mi></msub></mrow></math></span>’, which corroborated the increased relaxation time and existence of shallow trap state for x = 0.1 with that of <span><math><mrow><msub><mi>τ</mi><mi>z</mi></msub></mrow></math></span>. The respective activation energies are 0.37 eV, 0.44 eV, 0.79 eV and 0.034 eV for x = 0, 0.05, 0.1 and shallow trap state of x = 0.1 respectively. DC conduction also follo
采用溶胶-凝胶自燃烧法合成了La2Co1-xZnxMnO6 (x = 0,0.05和0.1)样品,并对其进行了系统表征。室温x射线衍射的Rietveld细化证实了一个单相单斜结构(空间群P21/n),在5% Zn取代时晶格参数的变化可以忽略不计,但在10% Zn取代时晶格参数明显膨胀。FESEM图像分析显示,掺杂Zn后,平均晶粒尺寸分别增加了112±35 nm (x = 0)、121±36 nm (x = 0.05)和187±66 nm (x = 0.1),孔隙率分别降低了15.3% (x = 0)、14% (x = 0.05)和5.74% (x = 0.1)。使用Havriliak-Negami模型分析阻抗谱,得到电阻(R)、弛豫时间(τZ)、不对称性(α)和宽度(β)参数,表明10%掺杂样品在所有温度下R和τZ都显著上升。从温度相关的“R”测量的交流电输运遵循可变范围跳变(VRH),当x = 0、0.05和0.1时,莫特温度(T0)分别为1.186 × 109 K、1.54 × 109 K和6.568 × 109 K。费米能级载流子的态密度为2.34×1019 ev−1。当x = 0时Cm−3,1.83×1019 ev−1。当x = 0.05和3.60×1018 ev−1时Cm−3。当x = 0.1时Cm−3。在温度范围为303 K - 363 K,活化能为0.049 eV τz的10%掺杂样品中,发现了与浅层供体捕获态有关的导通交叉,表现出热激活行为,活化能(Ea)值为0.33 eV (x = 0), 0.35 eV (x = 0.05)和0.53 eV (x = 0.1)。浅阱态也见于温度相关τz在x = 0.1时的值为0.041 eV。用Kohlrausch-Williams-Watts函数拟合的模量谱计算出τm,证实了x = 0.1时弛豫时间的增加和浅阱态的存在。x = 0、0.05、0.1和x = 0.1的浅阱态活化能分别为0.37 eV、0.44 eV、0.79 eV和0.034 eV。当x = 0、0.05和0.1时,直流导通也紧随VRH, T0值分别为1.28×108 K、1.96×108 K和4.60×108 K。在α, β和标度形式的所有成分中都观察到明显的非debye型弛豫行为。电介质研究表明,锌取代后介电常数(εr)和损耗(D)有系统的降低。随着Zn的取代,本征εr和D的温度窗增大。Cole-Cole分析进一步揭示了10%掺杂样品对应的低频麦克斯韦-瓦格纳贡献和高频浅阱态的高分辨半圆。
{"title":"Structural, microstructural, impedance spectroscopy and dielectric studies on La2Co1-xZnxMnO6 (x=0, 0.05 and 0.1) double perovskite","authors":"Swagatika Mohanty ,&nbsp;A.K. Biswal ,&nbsp;J. Ray","doi":"10.1016/j.jpcs.2025.113497","DOIUrl":"10.1016/j.jpcs.2025.113497","url":null,"abstract":"&lt;div&gt;&lt;div&gt;La&lt;sub&gt;2&lt;/sub&gt;Co&lt;sub&gt;1-x&lt;/sub&gt;Zn&lt;sub&gt;x&lt;/sub&gt;MnO&lt;sub&gt;6&lt;/sub&gt; (x = 0, 0.05 and 0.1) samples were synthesized via the sol–gel auto-combustion method and systematically characterized. Rietveld refinement of room-temperature X-ray diffraction confirmed a single-phase monoclinic structure (space group &lt;em&gt;P2&lt;/em&gt;&lt;sub&gt;&lt;em&gt;1&lt;/em&gt;&lt;/sub&gt;&lt;em&gt;/n&lt;/em&gt;), with negligible change in lattice parameters at 5 % Zn substitution but a pronounced expansion at 10 %. Analysis of FESEM images revealed the increase in average grain sizes: 112 ± 35 nm (x = 0), 121 ± 36 nm (x = 0.05) and 187 ± 66 nm (x = 0.1), with reduced porosity:15.3 % (x = 0), 14 % (x = 0.05) and 5.74 % (x = 0.1) upon Zn doping. Impedance spectra analysed using the Havriliak–Negami model yielded resistance (R), relaxation time (&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;τ&lt;/mi&gt;&lt;mi&gt;Z&lt;/mi&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;), asymmetry (α), and broadness (β) parameters, showing a significant rise in R and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;τ&lt;/mi&gt;&lt;mi&gt;z&lt;/mi&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; for the 10 % doped sample across all temperatures. A.C. electrical transport examined from temperature dependent ‘R’ followed variable-range hopping (VRH), with Mott temperatures (&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;) of 1.186 × 10&lt;sup&gt;9&lt;/sup&gt; K, 1.54 × 10&lt;sup&gt;9&lt;/sup&gt; K, and 6.568 × 10&lt;sup&gt;9&lt;/sup&gt; K for x = 0, 0.05, and 0.1, respectively. Density of states of the charge carriers at the Fermi level are &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;2.34&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mn&gt;19&lt;/mn&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; ev&lt;sup&gt;−1&lt;/sup&gt;.cm&lt;sup&gt;−3&lt;/sup&gt; for x = 0, &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;1.83&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mn&gt;19&lt;/mn&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; ev&lt;sup&gt;−1&lt;/sup&gt;.cm&lt;sup&gt;−3&lt;/sup&gt; for x = 0.05 and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;3.60&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mn&gt;18&lt;/mn&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; ev&lt;sup&gt;−1&lt;/sup&gt;.cm&lt;sup&gt;−3&lt;/sup&gt; for x = 0.1. A conduction crossover pertaining to trapped state of shallow donors was observed in the 10 % doped sample between temperature range 303 K–363 K with activation energy 0.049 eV &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;τ&lt;/mi&gt;&lt;mi&gt;z&lt;/mi&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; shows thermally activated behaviour with Activation energy (&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;E&lt;/mi&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;) values 0.33 eV (x = 0), 0.35 eV (x = 0.05) and 0.53 eV (x = 0.1). Shallow trap state is also seen in temperature dependent &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;τ&lt;/mi&gt;&lt;mi&gt;z&lt;/mi&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; for x = 0.1 has value 0.041 eV. Modulus spectra fitted with the Kohlrausch–Williams–Watts function calculated ‘&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;τ&lt;/mi&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;’, which corroborated the increased relaxation time and existence of shallow trap state for x = 0.1 with that of &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;τ&lt;/mi&gt;&lt;mi&gt;z&lt;/mi&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. The respective activation energies are 0.37 eV, 0.44 eV, 0.79 eV and 0.034 eV for x = 0, 0.05, 0.1 and shallow trap state of x = 0.1 respectively. DC conduction also follo","PeriodicalId":16811,"journal":{"name":"Journal of Physics and Chemistry of Solids","volume":"211 ","pages":"Article 113497"},"PeriodicalIF":4.9,"publicationDate":"2025-12-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145880471","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Band structure of structural fragments in Zr0·25Ti0·75Se2 Zr0·25Ti0·75Se2中结构碎片的能带结构
IF 4.9 3区 材料科学 Q2 CHEMISTRY, MULTIDISCIPLINARY Pub Date : 2025-12-23 DOI: 10.1016/j.jpcs.2025.113496
A.I. Merentsov , A.S. Shkvarin , M.S. Postnikov , A. Yu Kuznetsova , P. Dudin , J. Avila , A.N. Titov
The nano-ARPES experiment in combination with scanning photoelectron microscopy (SPEM) measurements provided nanoscale visualization of “pseudodoping” and insight into the electronic structure of the Zr0·25Ti0·75Se2 mixed crystal with inhomogeneous morphology. Using SPEM and Nano-ARPES we found the formation of the TiSe2-based and ZrSe2-based coherently bonded structural fragments. The appearance of the electron pocket in the M′ point of the Brillouin zone of TiSe2-based fragment confirmed the charge transfer from the ZrSe2-based fragments, which suppress charge-density-wave transition in TiSe2-based fragments.
纳米arpes实验与扫描光电子显微镜(SPEM)测量相结合,提供了“假掺杂”的纳米尺度可视化,并深入了解了非均匀形貌的Zr0·25Ti0·75Se2混合晶体的电子结构。通过SPEM和Nano-ARPES,我们发现形成了tise2基和zrse2基的结构片段。在tise2基碎片布里渊区M′点出现电子口袋,证实了zrse2基碎片的电荷转移,从而抑制了tise2基碎片中的电荷密度波跃迁。
{"title":"Band structure of structural fragments in Zr0·25Ti0·75Se2","authors":"A.I. Merentsov ,&nbsp;A.S. Shkvarin ,&nbsp;M.S. Postnikov ,&nbsp;A. Yu Kuznetsova ,&nbsp;P. Dudin ,&nbsp;J. Avila ,&nbsp;A.N. Titov","doi":"10.1016/j.jpcs.2025.113496","DOIUrl":"10.1016/j.jpcs.2025.113496","url":null,"abstract":"<div><div>The nano-ARPES experiment in combination with scanning photoelectron microscopy (SPEM) measurements provided nanoscale visualization of “pseudodoping” and insight into the electronic structure of the Zr<sub>0</sub><sub>·</sub><sub>25</sub>Ti<sub>0</sub><sub>·</sub><sub>75</sub>Se<sub>2</sub> mixed crystal with inhomogeneous morphology. Using SPEM and Nano-ARPES we found the formation of the TiSe<sub>2</sub>-based and ZrSe<sub>2</sub>-based coherently bonded structural fragments. The appearance of the electron pocket in the <em>M′</em> point of the Brillouin zone of TiSe<sub>2</sub>-based fragment confirmed the charge transfer from the ZrSe<sub>2</sub>-based fragments, which suppress charge-density-wave transition in TiSe<sub>2</sub>-based fragments.</div></div>","PeriodicalId":16811,"journal":{"name":"Journal of Physics and Chemistry of Solids","volume":"211 ","pages":"Article 113496"},"PeriodicalIF":4.9,"publicationDate":"2025-12-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145836897","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
High-fidelity modeling and validation of triple-absorber solar cell with post-transition metal perovskite absorbers 过渡后金属钙钛矿三吸收体太阳能电池的高保真建模与验证
IF 4.9 3区 材料科学 Q2 CHEMISTRY, MULTIDISCIPLINARY Pub Date : 2025-12-23 DOI: 10.1016/j.jpcs.2025.113492
Venkateswarlu G. , C.V.M. Chaturvedi , E. Sampad , Umakanta Nanda , J. Bhaskara Rao , Chih-Chieh Hsu
The transition towards eco-friendly and lead-free photovoltaic technologies has accelerated research into post-transition metal halide absorbers for their favorable optoelectronic properties with environmental safety. In this work, we propose a novel Triple-Absorber Post-Transition Metal Architecture (TAPTMA) comprised of FTO/SnO2/Cs3Bi2Br9/Cs2AgSbBr6/CsSnGeI3/P3HT. This configuration has SnO2 as the electron transport layer, P3HT as the hole transport layer, and an absorber Cs3Bi2Br9 interlayer to help efficient band alignment and charge transfer between sub-cells. SCAPS-1D simulation results show an open-circuit voltage (Voc) of 1.12 V, a short-circuit current density (Jsc) of 36.02 mA/cm2, a fill factor (FF) of 87.29%, and a power conversion efficiency (PCE) of 35.21%. These high-performance values come from the complementary optical absorption of the absorber layers, which enables broad-spectrum light absorption and reduced thermalization losses. The proposed TAPTMA’s non-toxic composition with optimized interfacial engineering, and superior efficiency positions it as a strong candidate for next-generation, stable, and environmentally friendly photovoltaics.
向环保和无铅光伏技术的过渡加速了过渡后金属卤化物吸收剂的研究,因为它们具有良好的光电性能和环境安全。在这项工作中,我们提出了一种由FTO/SnO2/Cs3Bi2Br9/Cs2AgSbBr6/CsSnGeI3/P3HT组成的新型三重吸收后过渡金属结构(TAPTMA)。该结构以SnO2作为电子传输层,P3HT作为空穴传输层,以及吸收剂Cs3Bi2Br9中间层来帮助有效的带对准和子电池之间的电荷转移。SCAPS-1D仿真结果表明,该电路的开路电压(Voc)为1.12 V,短路电流密度(Jsc)为36.02 mA/cm2,填充系数(FF)为87.29%,功率转换效率(PCE)为35.21%。这些高性能值来自吸收层的互补光学吸收,这使得广谱光吸收和减少热化损失。所提出的TAPTMA的无毒组合物具有优化的界面工程和优越的效率,使其成为下一代,稳定和环境友好型光伏电池的有力候选。
{"title":"High-fidelity modeling and validation of triple-absorber solar cell with post-transition metal perovskite absorbers","authors":"Venkateswarlu G. ,&nbsp;C.V.M. Chaturvedi ,&nbsp;E. Sampad ,&nbsp;Umakanta Nanda ,&nbsp;J. Bhaskara Rao ,&nbsp;Chih-Chieh Hsu","doi":"10.1016/j.jpcs.2025.113492","DOIUrl":"10.1016/j.jpcs.2025.113492","url":null,"abstract":"<div><div>The transition towards eco-friendly and lead-free photovoltaic technologies has accelerated research into post-transition metal halide absorbers for their favorable optoelectronic properties with environmental safety. In this work, we propose a novel Triple-Absorber Post-Transition Metal Architecture (TAPTMA) comprised of FTO/SnO<sub>2</sub>/Cs<sub>3</sub>Bi<sub>2</sub>Br<sub>9</sub>/Cs<sub>2</sub>AgSbBr<sub>6</sub>/CsSnGeI<sub>3</sub>/P3HT. This configuration has SnO<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span> as the electron transport layer, P3HT as the hole transport layer, and an absorber Cs<sub>3</sub>Bi<sub>2</sub>Br<sub>9</sub> interlayer to help efficient band alignment and charge transfer between sub-cells. SCAPS-1D simulation results show an open-circuit voltage (Voc) of 1.12 V, a short-circuit current density (Jsc) of 36.02 mA/cm<sup>2</sup>, a fill factor (FF) of 87.29%, and a power conversion efficiency (PCE) of 35.21%. These high-performance values come from the complementary optical absorption of the absorber layers, which enables broad-spectrum light absorption and reduced thermalization losses. The proposed TAPTMA’s non-toxic composition with optimized interfacial engineering, and superior efficiency positions it as a strong candidate for next-generation, stable, and environmentally friendly photovoltaics.</div></div>","PeriodicalId":16811,"journal":{"name":"Journal of Physics and Chemistry of Solids","volume":"211 ","pages":"Article 113492"},"PeriodicalIF":4.9,"publicationDate":"2025-12-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145836895","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Synergistic structural-electrochemical enhancement in ternary perovskite BiCrO3/GO/PANI over the binary BiCrO3/GO system for high-performance supercapacitors 三元钙钛矿BiCrO3/GO/PANI体系对高性能超级电容器的协同结构-电化学增强
IF 4.9 3区 材料科学 Q2 CHEMISTRY, MULTIDISCIPLINARY Pub Date : 2025-12-23 DOI: 10.1016/j.jpcs.2025.113470
Aisha Siddiqa , Malika Rani , Aqeel Ahmad Shah , Akram Ibrahim
The escalating global shift toward renewable energy has underscored the need for efficient and durable energy storage systems. Supercapacitors, owing to their rapid charge–discharge capability and long life cycle, offer an attractive route toward sustainable power technologies. In this study, BiCrO3 perovskite nanocomposite was integrated with graphene oxide (GO) 2D material, via the co-precipitation method and a Bismuth Cromiam oxide Perovskite/graphene oxide/Polyaniline (BiCrO3/GO/PANI) ternary nanocomposite was synthesized via situ-polymerization method to assess superior electrochemical performance. Structural, morphological, and surface characteristics were analyzed using XRD, SEM and FT-IR techniques. Electrochemical performance was evaluated using CV, GCD, and EIS analyses. Integration of GO enhanced redox activity and surface area, enabling a high specific capacitance of 1580 F g−1 at 2 A g−1 along with an energy density of 169.96 Wh kg−1 and power density of 1648 W kg−1. The BiCrO3/GO/PANI ternary electrode exhibited excellent performance, delivering a specific capacitance of 1980 F g−1, an energy density of 205.04 Wh kg−1, and a power density of 1654 W kg−1, with 90.9 % capacitance retention after 1000 cycles. EIS results of ternary nanocomposite revealed reduced charge-transfer impedence and internal resistance, confirming the nanocomposite's superior conductivity and stability in high-performance energy storage applications.
全球向可再生能源的不断升级,凸显了对高效、耐用的能源存储系统的需求。超级电容器由于其快速充放电能力和长寿命周期,为可持续电力技术提供了一条有吸引力的途径。本研究将BiCrO3钙钛矿纳米复合材料与氧化石墨烯(GO)二维材料结合,通过共沉淀法,通过原位聚合法制备了铋铬氧化物钙钛矿/氧化石墨烯/聚苯胺(BiCrO3/GO/PANI)三元纳米复合材料,以评价其优异的电化学性能。利用XRD、SEM和FT-IR技术分析了材料的结构、形貌和表面特征。电化学性能通过CV、GCD和EIS分析进行评价。氧化石墨烯的集成增强了氧化还原活性和表面积,在2 a g−1时实现了1580 F g−1的高比电容,以及169.96 Wh kg−1的能量密度和1648 W kg−1的功率密度。BiCrO3/GO/PANI三元电极表现出优异的性能,比电容为1980 F g−1,能量密度为205.04 Wh kg−1,功率密度为1654 W kg−1,循环1000次后电容保持率为90.9%。EIS结果显示,三元纳米复合材料的电荷转移阻抗和内阻降低,证实了纳米复合材料在高性能储能应用中的优越导电性和稳定性。
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引用次数: 0
Performance analysis of halide perovskites Be3NX3 (X=F, Cl, Br) with multiple hole and electron transport layers using DFT, SCAPS-1D and deep learning methods 利用DFT、SCAPS-1D和深度学习方法分析具有多空穴和电子传输层的卤化物钙钛矿Be3NX3 (X=F, Cl, Br)的性能
IF 4.9 3区 材料科学 Q2 CHEMISTRY, MULTIDISCIPLINARY Pub Date : 2025-12-23 DOI: 10.1016/j.jpcs.2025.113493
Indrojit Paul , Bipul Chandra Biswas , Asadul Islam Shimul , S. AlFaify , A.M. Elbasiony , Mohamed Benghanem , Md. Azizur Rahman
Concerns about the environment have led to a shift in focus from lead-based perovskite solar cells (PSCs) to safer alternatives such as Be3NX3 (X = F, Cl, Br). This research uses density functional theory (DFT) to examine the structural, electrical, and optical properties, with a particular focus on environmental safety and light-harvesting efficiency. The band gaps determined using GGA-PBE techniques were 6.255 eV for Be3NF3, 1.476 eV for Be3NCl3, and 0.484 eV for Be3NBr3. The bandgap of Be3NCl3 is located within the ideal range (0.8–2.2 eV) for photovoltaic applications, making it a potential candidate. The SCAPS-1D simulator was utilized to assess several device designs incorporating various hole transport layers (HTLs) and electron transport layers (ETLs). Out of the 30 configurations that were evaluated, the Al/FTO/SnS2/Be3NCl3/Cu2O/Ni arrangement attained an open-circuit voltage (VOC) of 1.1781 V, a peak power conversion efficiency (PCE) of 29.90 %, with a fill factor (FF) of 88.85 %, and a short-circuit current density (JSC) of 28.5621 mA/cm2. Furthermore, this research employs eight deep learning algorithms to evaluate and classify the design variables that most significantly impact key performance metrics, particularly PCE. The Bidirectional GRU (BiGRU) model is distinguished by its superior performance, attaining a mean squared error (MSE) of 1.422 and a remarkable R2 value of 0.98, so establishing itself as the most precise model for performance prediction. In addition, the investigation evaluates the influence of material properties on the model's output, highlighting the substantial impact of the defect density and absorbent section characteristics on the overall efficiency. These findings provide significant insights for experimental researchers, facilitating the advancement of extremely efficient and cost-effective solar technologies.
对环境的担忧导致人们将重点从铅基钙钛矿太阳能电池(PSCs)转向更安全的替代品,如Be3NX3 (X = F, Cl, Br)。本研究使用密度泛函理论(DFT)来检查结构,电学和光学性质,特别关注环境安全和光收集效率。采用GGA-PBE技术测定的带隙分别为Be3NF3的6.255 eV、Be3NCl3的1.476 eV和Be3NBr3的0.484 eV。Be3NCl3的带隙位于光伏应用的理想范围内(0.8-2.2 eV),使其成为潜在的候选材料。利用SCAPS-1D模拟器评估了几种包含不同空穴传输层(HTLs)和电子传输层(ETLs)的器件设计。在30种结构中,Al/FTO/SnS2/Be3NCl3/Cu2O/Ni结构的开路电压(VOC)为1.1781 V,峰值功率转换效率(PCE)为29.90%,填充系数(FF)为88.85%,短路电流密度(JSC)为28.5621 mA/cm2。此外,本研究采用8种深度学习算法对影响关键性能指标(尤其是PCE)的设计变量进行评估和分类,其中双向GRU (BiGRU)模型具有优异的性能,均方误差(MSE)为1.422,R2为0.98,是最精确的性能预测模型。此外,研究还评估了材料性能对模型输出的影响,突出了缺陷密度和吸收截面特性对整体效率的重大影响。这些发现为实验研究人员提供了重要的见解,促进了极其高效和具有成本效益的太阳能技术的发展。
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引用次数: 0
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Journal of Physics and Chemistry of Solids
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