We report a comprehensive investigation of the third-order nonlinear interaction of femtosecond laser pulses with nanostructured anatase TiO2 doped with varying concentrations of gadolinium impurities. The samples were synthesized using a facile sol‒gel method. The physicochemical characteristics of the prepared samples were investigated using various analytical techniques, including XRD, SEM, TEM, SAED, UV‒Vis, PL and XPS. The average crystallite sizes of the pristine TiO2- and Gd (1, 2, and 3 %)-doped TiO2 nanoparticles were calculated to be 10.9, 9.2, 10.2 and 8.9 nm, respectively. The W-H plots also revealed average crystallite sizes in the range of 13.9, 16.6, 13.9 and 10.4 for pristine and Gd (1, 2, 3 %)-doped TiO2 nanoparticles. The lattice strain values for pristine and Gd (1, 2, and 3 %) doped TiO2 nanoparticles were computed as 0.00203, 0.00667, 0.0036 and 0.00262, respectively, from the W‒H plots. The average crystallite size was calculated to 9.2 nm from the TEM images using ImageJ software. The optical band gap values of pristine TiO2 and Gd (1, 2, and 3 %)-doped TiO2 nanoparticles were calculated to be 3.3, 3.23, 3.21 and 3.20 eV from the Kubelka–Munk function plot. The emission peaks of pristine and Gd(1,2,3 %) doped TiO2 nanoparticles were calculated as 3.2, 3.23, 3.26 and 3.32 eV from the photoluminescence spectra recorded at 330 nm photo excitation. The binding energies of the O1s, Ti2P and Gd4d peaks present in the survey scan of TiO2 nanoparticles doped with one weight percentage of Gd impurity were 528.79, 531.53, 457.53, 463.25 and 149.6 eV, respectively. The third-order nonlinear characteristics of the TiO2:Gd samples were probed using the ultrafast laser Z-scan technique. We observed that the density of bound excitons can be regulated by controlling the dopant concentration. The strong oscillatory interactions between photogenerated bound excitons, which act as dipole oscillators with large oscillating frequencies, were recorded using a single-beam femtosecond Z-scan. The third-order nonlinear susceptibility χ(3) for pristine and Gd(1,2,3 %)-doped TiO2 nanoparticles were calculated as 7.258 × 10-18, 9.4 × 10-18, 11 × 10-18 and 13 × 10-18 cm2/V2, respectively. The obtained results suggest that the thermal lensing phenomenon in nanostructured anatase TiO2 can be generated and effectively controlled using a band gap engineering technique. We determined that the small pump power in nonlinear media with controllable band fluctuations can produce large phase distortions in TiO2:Gd nanosystems. Our findings reveal that Gd doping induces controlled modification of the electronic structure of TiO2, leading to a tailored energy landscape for exciton formation and binding. These findings provide a novel approa
{"title":"Bound exciton engineering approach for tuning the thermal lensing phenomenon in anatase TiO2: Gd nanosystems","authors":"Oriparambil Sivaraman Nirmal Ghosh , Sethuraman Gayathri , Srinivasa Rao Allam , Alok Sharan , S.B. Sruthil Lal , Modigunta Jeevan Kumar Reddy , A.M. Shanmugharaj , Annamraju Kasi Viswanath","doi":"10.1016/j.chphi.2024.100679","DOIUrl":"https://doi.org/10.1016/j.chphi.2024.100679","url":null,"abstract":"<div><p>We report a comprehensive investigation of the third-order nonlinear interaction of femtosecond laser pulses with nanostructured anatase TiO<sub>2</sub> doped with varying concentrations of gadolinium impurities. The samples were synthesized using a facile sol‒gel method. The physicochemical characteristics of the prepared samples were investigated using various analytical techniques, including XRD, SEM, TEM, SAED, UV‒Vis, PL and XPS. The average crystallite sizes of the pristine TiO<sub>2-</sub> and Gd (1, 2, and 3 %)-doped TiO<sub>2</sub> nanoparticles were calculated to be 10.9, 9.2, 10.2 and 8.9 nm, respectively. The W-H plots also revealed average crystallite sizes in the range of 13.9, 16.6, 13.9 and 10.4 for pristine and Gd (1, 2, 3 %)-doped TiO<sub>2</sub> nanoparticles. The lattice strain values for pristine and Gd (1, 2, and 3 %) doped TiO<sub>2</sub> nanoparticles were computed as 0.00203, 0.00667, 0.0036 and 0.00262, respectively, from the W‒H plots. The average crystallite size was calculated to 9.2 nm from the TEM images using ImageJ software. The optical band gap values of pristine TiO<sub>2</sub> and Gd (1, 2, and 3 %)-doped TiO<sub>2</sub> nanoparticles were calculated to be 3.3, 3.23, 3.21 and 3.20 eV from the Kubelka–Munk function plot. The emission peaks of pristine and Gd(1,2,3 %) doped TiO<sub>2</sub> nanoparticles were calculated as 3.2, 3.23, 3.26 and 3.32 eV from the photoluminescence spectra recorded at 330 nm photo excitation. The binding energies of the O1s, Ti2P and Gd4d peaks present in the survey scan of TiO<sub>2</sub> nanoparticles doped with one weight percentage of Gd impurity were 528.79, 531.53, 457.53, 463.25 and 149.6 eV, respectively. The third-order nonlinear characteristics of the TiO<sub>2</sub>:Gd samples were probed using the ultrafast laser Z-scan technique. We observed that the density of bound excitons can be regulated by controlling the dopant concentration. The strong oscillatory interactions between photogenerated bound excitons, which act as dipole oscillators with large oscillating frequencies, were recorded using a single-beam femtosecond Z-scan. The third-order nonlinear susceptibility χ(3) for pristine and Gd(1,2,3 %)-doped TiO<sub>2</sub> nanoparticles were calculated as 7.258 × 10<sup>-18</sup>, 9.4 × 10<sup>-18</sup>, 11 × 10<sup>-18</sup> and 13 × 10<sup>-18</sup> cm<sup>2</sup>/V<sup>2</sup>, respectively. The obtained results suggest that the thermal lensing phenomenon in nanostructured anatase TiO<sub>2</sub> can be generated and effectively controlled using a band gap engineering technique. We determined that the small pump power in nonlinear media with controllable band fluctuations can produce large phase distortions in TiO<sub>2</sub>:Gd nanosystems. Our findings reveal that Gd doping induces controlled modification of the electronic structure of TiO<sub>2</sub>, leading to a tailored energy landscape for exciton formation and binding. These findings provide a novel approa","PeriodicalId":9758,"journal":{"name":"Chemical Physics Impact","volume":null,"pages":null},"PeriodicalIF":3.8,"publicationDate":"2024-07-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2667022424002238/pdfft?md5=a37f00c5d6cb58c275e78d76ad972651&pid=1-s2.0-S2667022424002238-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141593542","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-05DOI: 10.1016/j.chphi.2024.100676
S. Abinaya , R. Sakthivel , K. Ramachandran , P.M. Vivek , Mohamed Arfayeen , C.S. Manikandababu , R. BoopathiRaja
Exploiting efficient Pt-free counter-electrode materials with low cost and highly catalytic property is a hot topic in the field of Dye-sensitized solar cells (DSCs). Here, NiCo2S4/reduced graphene oxide (RGO) was prepared via an economical hydrothermal ynthesis route, and the as-prepared composite exhibited comparable electrocatalytic property with the conventional Pt electrode as the counter-electrode. Enhanced optoelectronic, optical and structural characteristics have been attained over the constructed heterojunction. Band gap energy of NiCo2S4 (2.35 eV) was suppressed to 2.11 eV owing to its supporting with 10 wt.% rGO bringing about upgraded absorption of visible light. Electrochemical studies confirmed the synergetic effect of nickel and cobalt ions with the high electrical conductive rGO networks that enhance the electrocatalytic activity of NiCo2S4 nanostructures. The efficiency achieved for the NiCo2S4@rGO counter electrode (CE) based DSSC is 8.17%, which is remarkably higher than that of pristine NiCo2S4 (7.31%), and Pt (7.14%) under the same experimental conditions. In outline, given their innovative synthesis approach, affordability, and remarkable electrocatalytic attributes, the newly developed NiCo2S4@rGO counter electrodes stand out as potent contenders in future dye-sensitized solar cell applications.
{"title":"Design and fabrication of NiCo2S4@rGO as an efficient Pt free triiodide reducing agent for dye-sensitized solar cell application","authors":"S. Abinaya , R. Sakthivel , K. Ramachandran , P.M. Vivek , Mohamed Arfayeen , C.S. Manikandababu , R. BoopathiRaja","doi":"10.1016/j.chphi.2024.100676","DOIUrl":"10.1016/j.chphi.2024.100676","url":null,"abstract":"<div><p>Exploiting efficient Pt-free counter-electrode materials with low cost and highly catalytic property is a hot topic in the field of Dye-sensitized solar cells (DSCs). Here, NiCo<sub>2</sub>S<sub>4</sub>/reduced graphene oxide (RGO) was prepared via an economical hydrothermal ynthesis route, and the as-prepared composite exhibited comparable electrocatalytic property with the conventional Pt electrode as the counter-electrode. Enhanced optoelectronic, optical and structural characteristics have been attained over the constructed heterojunction. Band gap energy of NiCo<sub>2</sub>S<sub>4</sub> (2.35 eV) was suppressed to 2.11 eV owing to its supporting with 10 wt.% rGO bringing about upgraded absorption of visible light. Electrochemical studies confirmed the synergetic effect of nickel and cobalt ions with the high electrical conductive rGO networks that enhance the electrocatalytic activity of NiCo<sub>2</sub>S<sub>4</sub> nanostructures. The efficiency achieved for the NiCo<sub>2</sub>S<sub>4</sub>@rGO counter electrode (CE) based DSSC is 8.17%, which is remarkably higher than that of pristine NiCo<sub>2</sub>S<sub>4</sub> (7.31%), and Pt (7.14%) under the same experimental conditions. In outline, given their innovative synthesis approach, affordability, and remarkable electrocatalytic attributes, the newly developed NiCo<sub>2</sub>S<sub>4</sub>@rGO counter electrodes stand out as potent contenders in future dye-sensitized solar cell applications.</p></div>","PeriodicalId":9758,"journal":{"name":"Chemical Physics Impact","volume":null,"pages":null},"PeriodicalIF":3.8,"publicationDate":"2024-07-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2667022424002202/pdfft?md5=ad37a648c4b17e8e0ef21fab371f04f9&pid=1-s2.0-S2667022424002202-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141694387","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-05DOI: 10.1016/j.chphi.2024.100681
Nithya S. George , Riya Mary Cherian , D.A. Nayana , Dinesh Raj R , Ramesh T Subramaniam , Arun Aravind
Water contamination resulting from the presence of organic dye pollutants in the ecosystem is a significant issue in the 21st century, that requires urgent resolution. Utilizing an effective nanocatalyst for the removal of dyes from water is a viable solution to address this problem. In this study, we proposed two distinct approaches for synthesizing δ-MnO2 nanostructures: an environmentally friendly, “green” method (MG) and a “cost-effective” hydrothermal method (MH). The leaf extract of Clinacanthus nutans was used for the preparation of MG, while MnSO4 was used for MH as a reducing agent, along with KMnO4, with the reaction time fixed at 90 °C. X-ray diffraction analysis confirmed that both approaches yielded δ-MnO2 nanostructures with a monoclinic Birnessite phase. The MG sample displayed a coagulated nanoflake-like morphology, as observed in FESEM images. On the other hand, the MH sample exhibited a distinct nanoflower morphology. The materials' optical properties were investigated using UV–visible spectra analysis, revealing direct bandgap energies of 2.2 eV and 2.58 eV for the MG and MH, respectively. The surface area of the MG sample was found to be higher as compared to the MH nanoflower, showcasing a mesoporous structure. XPS analysis was employed to determine the oxidation states of the elements. The effect of varying pH levels on the degradation of Methyl Orange dye by the two nanocatalysts was investigated. The results demonstrated that acidic pH led to higher decolouration efficiency, particularly notable for the MG nanocatalyst. Consequently, this study illustrates that the green δ-MnO2 nanocatalyst effectively degrades methyl orange dye under acidic conditions through photocatalysis.
{"title":"Birnessite-MnO2 nanostructures synthesized by facile hydrothermal and green method for dye degradation application","authors":"Nithya S. George , Riya Mary Cherian , D.A. Nayana , Dinesh Raj R , Ramesh T Subramaniam , Arun Aravind","doi":"10.1016/j.chphi.2024.100681","DOIUrl":"https://doi.org/10.1016/j.chphi.2024.100681","url":null,"abstract":"<div><p>Water contamination resulting from the presence of organic dye pollutants in the ecosystem is a significant issue in the 21st century, that requires urgent resolution. Utilizing an effective nanocatalyst for the removal of dyes from water is a viable solution to address this problem. In this study, we proposed two distinct approaches for synthesizing δ-MnO<sub>2</sub> nanostructures: an environmentally friendly, “green” method (MG) and a “cost-effective” hydrothermal method (MH). The leaf extract of <em>Clinacanthus nutans</em> was used for the preparation of MG, while MnSO<sub>4</sub> was used for MH as a reducing agent, along with KMnO<sub>4</sub>, with the reaction time fixed at 90 °C. X-ray diffraction analysis confirmed that both approaches yielded δ-MnO<sub>2</sub> nanostructures with a monoclinic Birnessite phase. The MG sample displayed a coagulated nanoflake-like morphology, as observed in FESEM images. On the other hand, the MH sample exhibited a distinct nanoflower morphology. The materials' optical properties were investigated using UV–visible spectra analysis, revealing direct bandgap energies of 2.2 eV and 2.58 eV for the MG and MH, respectively. The surface area of the MG sample was found to be higher as compared to the MH nanoflower, showcasing a mesoporous structure. XPS analysis was employed to determine the oxidation states of the elements. The effect of varying pH levels on the degradation of Methyl Orange dye by the two nanocatalysts was investigated. The results demonstrated that acidic pH led to higher decolouration efficiency, particularly notable for the MG nanocatalyst. Consequently, this study illustrates that the green δ-MnO<sub>2</sub> nanocatalyst effectively degrades methyl orange dye under acidic conditions through photocatalysis.</p></div>","PeriodicalId":9758,"journal":{"name":"Chemical Physics Impact","volume":null,"pages":null},"PeriodicalIF":3.8,"publicationDate":"2024-07-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2667022424002251/pdfft?md5=c9253082709072c01caa5823a699aa0a&pid=1-s2.0-S2667022424002251-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141593541","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Magnetic garnets, a diverse group of magnetic insulating materials, have been the subject of extensive research for decades, owing to their versatility and potential for a wide range of applications. In this study, we synthesized Bismuth-Substituted Yttrium Iron Garnet (BiY2Fe5O12: BiYIG) using the solid-state reaction method to explore its structural, optical, and dielectric characteristics. X-ray diffraction analysis revealed the attainment of a pure cubic garnet phase in BiYIG, with a lattice parameter of 12.444 Å. Using UV–visible spectroscopy, we determined that the optical band gap of BiYIG is 2.2 eV, indicating n-type semiconductor behavior. We conducted a thorough investigation of the dielectric properties, examining capacitance, dielectric constant, dielectric loss, conductivity, impedance, and modulus, as functions of frequency and temperature. The impedance results revealed that the dielectric relaxation at room temperature was dominated by a Debye-type process, with a shift to a non-Debye-type process becoming apparent as temperature increased. Comprehensive analysis sheds light on the material's transport phenomena and optical attributes, offering insights into the potential of BiYIG for applications in magneto-dielectric and magneto-optical domains, given its high dielectric constant with low dielectric loss, and promising optical properties. These findings position BiYIG as a versatile material and underscore its suitability for advanced applications in future technological developments.
{"title":"Exploring bismuth-substituted yttrium iron garnet: Insights into structural, optical, and dielectric characteristics","authors":"Ravindra Hazam , Manjushree Maity , Sachin Verma, Rajeev Singh, Biswanath Bhoi","doi":"10.1016/j.chphi.2024.100671","DOIUrl":"https://doi.org/10.1016/j.chphi.2024.100671","url":null,"abstract":"<div><p>Magnetic garnets, a diverse group of magnetic insulating materials, have been the subject of extensive research for decades, owing to their versatility and potential for a wide range of applications. In this study, we synthesized Bismuth-Substituted Yttrium Iron Garnet (BiY<sub>2</sub>Fe<sub>5</sub>O<sub>12</sub>: BiYIG) using the solid-state reaction method to explore its structural, optical, and dielectric characteristics. X-ray diffraction analysis revealed the attainment of a pure cubic garnet phase in BiYIG, with a lattice parameter of 12.444 Å. Using UV–visible spectroscopy, we determined that the optical band gap of BiYIG is 2.2 eV, indicating n-type semiconductor behavior. We conducted a thorough investigation of the dielectric properties, examining capacitance, dielectric constant, dielectric loss, conductivity, impedance, and modulus, as functions of frequency and temperature. The impedance results revealed that the dielectric relaxation at room temperature was dominated by a Debye-type process, with a shift to a non-Debye-type process becoming apparent as temperature increased. Comprehensive analysis sheds light on the material's transport phenomena and optical attributes, offering insights into the potential of BiYIG for applications in magneto-dielectric and magneto-optical domains, given its high dielectric constant with low dielectric loss, and promising optical properties. These findings position BiYIG as a versatile material and underscore its suitability for advanced applications in future technological developments.</p></div>","PeriodicalId":9758,"journal":{"name":"Chemical Physics Impact","volume":null,"pages":null},"PeriodicalIF":3.8,"publicationDate":"2024-07-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2667022424002159/pdfft?md5=ff3bcde70dfc1e50887301c4f0da30ea&pid=1-s2.0-S2667022424002159-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141607497","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-03DOI: 10.1016/j.chphi.2024.100672
A. Bakour , M. Al-Hattab , O. Bajjou , K. Rahmani
This study presents a novel photovoltaic cell design utilizing a layered structure of Indium Tin Oxide (ITO), Zinc Selenide (ZnSe), and Carbon Nanotubes (CNTs) for enhanced solar energy conversion. We employed the Solar Cell Capacity Simulator (SCAPS-1D) to model and optimize the device under AM 1.5 spectrum conditions. Our simulations systematically investigated the influence of key parameters including layer thicknesses, doping concentrations, temperature, back contact work function, and parasitic resistances on cell performance. The optimized structure demonstrated a theoretical power conversion efficiency of 29.91%, with an open-circuit voltage (Voc) of 799 mV, a short-circuit current density (Jsc) of 43.49 mA/cm², and a fill factor (FF) of 86.02%. These promising results are attributed to the synergistic combination of CNTs' broad spectral absorption, ZnSe's effective charge separation, and optimized layer properties. We found that the CNT absorber layer's doping concentration significantly impacted cell performance, with an optimal value of 10¹⁷ cm⁻³. The ZnSe buffer layer thickness showed minimal effect on efficiency within the studied range. Temperature increases from 300 K to 400 K led to a significant efficiency drop from 33.97% to 24.65%, primarily due to Voc reduction. While these results represent idealized conditions and upper theoretical limits, they provide valuable insights for the potential of CNT-based solar cells. This study offers a roadmap for future experimental work in high-efficiency thin-film photovoltaics, highlighting the promise of novel material combinations and the importance of device architecture optimization.
{"title":"Efficiency enhancement of novel ITO/ZnSe/CNTs thin film solar cell","authors":"A. Bakour , M. Al-Hattab , O. Bajjou , K. Rahmani","doi":"10.1016/j.chphi.2024.100672","DOIUrl":"https://doi.org/10.1016/j.chphi.2024.100672","url":null,"abstract":"<div><p>This study presents a novel photovoltaic cell design utilizing a layered structure of Indium Tin Oxide (ITO), Zinc Selenide (ZnSe), and Carbon Nanotubes (CNTs) for enhanced solar energy conversion. We employed the Solar Cell Capacity Simulator (SCAPS-1D) to model and optimize the device under AM 1.5 spectrum conditions. Our simulations systematically investigated the influence of key parameters including layer thicknesses, doping concentrations, temperature, back contact work function, and parasitic resistances on cell performance. The optimized structure demonstrated a theoretical power conversion efficiency of 29.91%, with an open-circuit voltage (Voc) of 799 mV, a short-circuit current density (Jsc) of 43.49 mA/cm², and a fill factor (FF) of 86.02%. These promising results are attributed to the synergistic combination of CNTs' broad spectral absorption, ZnSe's effective charge separation, and optimized layer properties. We found that the CNT absorber layer's doping concentration significantly impacted cell performance, with an optimal value of 10¹⁷ cm⁻³. The ZnSe buffer layer thickness showed minimal effect on efficiency within the studied range. Temperature increases from 300 K to 400 K led to a significant efficiency drop from 33.97% to 24.65%, primarily due to Voc reduction. While these results represent idealized conditions and upper theoretical limits, they provide valuable insights for the potential of CNT-based solar cells. This study offers a roadmap for future experimental work in high-efficiency thin-film photovoltaics, highlighting the promise of novel material combinations and the importance of device architecture optimization.</p></div>","PeriodicalId":9758,"journal":{"name":"Chemical Physics Impact","volume":null,"pages":null},"PeriodicalIF":3.8,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2667022424002160/pdfft?md5=f16b48fe15349f7bbbb5d1bfae43db1a&pid=1-s2.0-S2667022424002160-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141593540","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
This study presents a planar hybrid system consisting of an electric-field-coupled resonator (ELCR) and yttrium iron garnet (YIG) film, designed to investigate the interaction between photons and magnons at room temperature. This hybrid system has been designed and simulated using the commercial electromagnetic full-wave simulator CST Microwave Studio. The phenomenon of anti-crossing between the photon mode of the ELCR and the magnon modes of the YIG was observed by analyzing the |S21|-versus-frequency spectrum under varying strengths of bias magnetic fields. We present a comprehensive theoretical framework that explains the observed anti-crossing effect resulting from photon-magnon coupling (PMC) and provide estimations for the strength of PMC (Δ). Additionally, the interaction between photons and magnons was manipulated through two distinct methods: by adjusting the thickness () of the YIG film and by positioning the YIG films along the microstripline. For the ELCR (for = 25 μm), Δ comes to 58 MHz, while changing from 2 μm to 50 μm, enabling more precise control of the Δ parameter across the span of 17 MHz to 84 MHz. Similarly, the YIG positioning at a different location along the microstripline allowed manipulation of Δ from 5 to 50 MHz. The resultant PMC can be significantly tuned by 400% to 900% in a planar-geometry ELCR-YIG hybrid system. This research offers avenues for developing innovative hybrid systems that afford greater control over the magnitude of PMC in a planar configuration, representing a promising direction for future advancements in hybrid magnonic systems.
{"title":"Room temperature photon-magnon coupling in YIG- electric field coupled resonator system","authors":"Abhishek Maurya , Kuldeep Kumar Shrivastava , Sachin Verma, Rajeev Singh, Biswanath Bhoi","doi":"10.1016/j.chphi.2024.100669","DOIUrl":"https://doi.org/10.1016/j.chphi.2024.100669","url":null,"abstract":"<div><p>This study presents a planar hybrid system consisting of an electric-field-coupled resonator (ELCR) and yttrium iron garnet (YIG) film, designed to investigate the interaction between photons and magnons at room temperature. This hybrid system has been designed and simulated using the commercial electromagnetic full-wave simulator CST Microwave Studio. The phenomenon of anti-crossing between the photon mode of the ELCR and the magnon modes of the YIG was observed by analyzing the |S<sub>21</sub>|-versus-frequency spectrum under varying strengths of bias magnetic fields. We present a comprehensive theoretical framework that explains the observed anti-crossing effect resulting from photon-magnon coupling (PMC) and provide estimations for the strength of PMC (Δ). Additionally, the interaction between photons and magnons was manipulated through two distinct methods: by adjusting the thickness (<span><math><msub><mi>t</mi><mtext>YIG</mtext></msub></math></span>) of the YIG film and by positioning the YIG films along the microstripline. For the ELCR (for <span><math><msub><mi>t</mi><mtext>YIG</mtext></msub></math></span> = 25 μm), Δ comes to 58 MHz, while changing <span><math><msub><mi>t</mi><mtext>YIG</mtext></msub></math></span> from 2 μm to 50 μm, enabling more precise control of the Δ parameter across the span of 17 MHz to 84 MHz. Similarly, the YIG positioning at a different location along the microstripline allowed manipulation of Δ from 5 to 50 MHz. The resultant PMC can be significantly tuned by 400% to 900% in a planar-geometry ELCR-YIG hybrid system. This research offers avenues for developing innovative hybrid systems that afford greater control over the magnitude of PMC in a planar configuration, representing a promising direction for future advancements in hybrid magnonic systems.</p></div>","PeriodicalId":9758,"journal":{"name":"Chemical Physics Impact","volume":null,"pages":null},"PeriodicalIF":3.8,"publicationDate":"2024-06-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2667022424002135/pdfft?md5=c8bf41a772433a9ece6a379d597099bc&pid=1-s2.0-S2667022424002135-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141605985","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-24DOI: 10.1016/j.chphi.2024.100670
Rahulkumar Shirasangi, Lakhanlal, Hari Prasad Dasari, M.B. Saidutta
Solid oxide electrolysis cells (SOECs) stabilize CO2 emissions by converting CO2/H2O into synfuel. Current-Voltage (i-V) characteristics of an electrolyte-supported button cell (NiO-YSZ/NiO-SDC/ScSZ/LSCF-GDC/LSCF) were measured as a function of temperature, water vapor concentration, and CO2 gas concentrations. The cell microstructure was characterized by the Field Emission Scanning Electron Microscope (FE-SEM). FE-SEM micrographs depict that the electrolyte layer is relatively dense, and porous fuel and air electrode layers are well adhered to the electrolyte. The i-V curves were obtained at a scan rate of 0.02 Vs−1 from 0.3 to 1.5 V. Electrolysis current density increases as the temperature increases. SOEC performance increases, but SOFC performance decreases with increased water vapor concentration. Electrolysis current densities decrease as the CO2 concentration increases. The i-V characteristics show only ohmic polarization under fuel-lean and fuel-rich conditions. At optimal conditions, current density values at 800 °C/1.5 V are -174, -187, and -195 mA cm−2 for 5 %H2O, 30 %CO2, and 30 %CO2/5 %H2O co-electrolysis. At 800 °C, open-circuit voltage (OCV) values for H2O, CO2, and co-electrolysis are 0.906, 0.891, and 0.885 V, respectively. The electrolysis area-specific resistances (ASRs) give information on the reduction of CO2 or H2O, forming CO or H2, respectively. At optimal conditions, ASR values are 3.43, 3.29, and 3.18 Ω cm2 for H2O, CO2, and co-electrolysis, respectively. Co-electrolysis has a lower ASR value than pure H2O and CO2 electrolysis, indicating that H2O and CO2 are involved in the electrochemical processes.
固体氧化物电解池(SOEC)通过将 CO2/H2O 转化为合成燃料来稳定二氧化碳的排放。测量了电解质支持的扣式电池(NiO-YSZ/NiO-SDC/ScSZ/LSCF-GDC/LSCF)的电流电压(i-V)特性与温度、水蒸气浓度和二氧化碳气体浓度的函数关系。电池的微观结构由场发射扫描电子显微镜(FE-SEM)进行表征。FE-SEM 显微照片显示,电解质层相对致密,多孔燃料层和空气电极层与电解质附着良好。在 0.02 Vs-1 的扫描速率下,获得了 0.3 至 1.5 V 的 i-V 曲线。电解电流密度随温度升高而增加。SOEC 性能随着水蒸气浓度的增加而提高,但 SOFC 性能则随着水蒸气浓度的增加而降低。电解电流密度随着二氧化碳浓度的增加而降低。在燃料贫乏和燃料丰富的条件下,i-V 特性只显示出欧姆极化。在最佳条件下,5 %H2O、30 %CO2 和 30 %CO2/5 %H2O 共电解在 800 °C/1.5 V 时的电流密度值分别为 -174、-187 和 -195 mA cm-2。800 °C 时,H2O、CO2 和共电解的开路电压 (OCV) 值分别为 0.906、0.891 和 0.885 V。电解区域特异电阻(ASR)提供了 CO2 或 H2O 还原成 CO 或 H2 的信息。在最佳条件下,H2O、CO2 和共电解的 ASR 值分别为 3.43、3.29 和 3.18 Ω cm2。共电解的 ASR 值低于纯 H2O 和 CO2 电解,表明 H2O 和 CO2 参与了电化学过程。
{"title":"Current-Voltage (i-V) characteristics of electrolyte-supported (NiO-YSZ/NiO-SDC/ScSZ/LSCF-GDC/LSCF) solid oxide electrolysis cell during CO2/H2O co-electrolysis","authors":"Rahulkumar Shirasangi, Lakhanlal, Hari Prasad Dasari, M.B. Saidutta","doi":"10.1016/j.chphi.2024.100670","DOIUrl":"https://doi.org/10.1016/j.chphi.2024.100670","url":null,"abstract":"<div><p>Solid oxide electrolysis cells (SOECs) stabilize CO<sub>2</sub> emissions by converting CO<sub>2</sub>/H<sub>2</sub>O into synfuel. Current-Voltage (i-V) characteristics of an electrolyte-supported button cell (NiO-YSZ/NiO-SDC/ScSZ/LSCF-GDC/LSCF) were measured as a function of temperature, water vapor concentration, and CO<sub>2</sub> gas concentrations. The cell microstructure was characterized by the Field Emission Scanning Electron Microscope (FE-SEM). FE-SEM micrographs depict that the electrolyte layer is relatively dense, and porous fuel and air electrode layers are well adhered to the electrolyte. The i-V curves were obtained at a scan rate of 0.02 Vs<sup>−1</sup> from 0.3 to 1.5 V. Electrolysis current density increases as the temperature increases. SOEC performance increases, but SOFC performance decreases with increased water vapor concentration. Electrolysis current densities decrease as the CO<sub>2</sub> concentration increases. The i-V characteristics show only ohmic polarization under fuel-lean and fuel-rich conditions. At optimal conditions, current density values at 800 °C/1.5 V are -174, -187, and -195 mA cm<sup>−2</sup> for 5 %H<sub>2</sub>O, 30 %CO<sub>2</sub>, and 30 %CO<sub>2</sub>/5 %H<sub>2</sub>O co-electrolysis. At 800 °C, open-circuit voltage (OCV) values for H<sub>2</sub>O, CO<sub>2</sub>, and co-electrolysis are 0.906, 0.891, and 0.885 V, respectively. The electrolysis area-specific resistances (ASRs) give information on the reduction of CO<sub>2</sub> or H<sub>2</sub>O, forming CO or H<sub>2</sub>, respectively. At optimal conditions, ASR values are 3.43, 3.29, and 3.18 Ω cm<sup>2</sup> for H<sub>2</sub>O, CO<sub>2</sub>, and co-electrolysis, respectively. Co-electrolysis has a lower ASR value than pure H<sub>2</sub>O and CO<sub>2</sub> electrolysis, indicating that H<sub>2</sub>O and CO<sub>2</sub> are involved in the electrochemical processes.</p></div>","PeriodicalId":9758,"journal":{"name":"Chemical Physics Impact","volume":null,"pages":null},"PeriodicalIF":3.8,"publicationDate":"2024-06-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2667022424002147/pdfft?md5=d00bbfa261dbd0b5f47c4b0175b4d674&pid=1-s2.0-S2667022424002147-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141482433","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-22DOI: 10.1016/j.chphi.2024.100663
R. Yuvashri , Era Dravida Thendral , D. Reuben Jonathan , A. Anish Fathima , K. Laavanya , G. Usha
In this work, a series of curcumin derivatives have been synthesized using Claisen Schmidt condensation reaction & Schotten-Baumann reaction, and they were screened through in-silico and in-vitro analysis to determine their capacity as a potential agent against breast cancer. Molecular docking reveals that the compounds are in good fit in the active site region of the target protein. Anti-cancer activity reveals that compounds are highly active against the MCF-7 cell lines, even at low concentration. Among the synthesized compounds, a set of five (Group B) exhibits a nontoxic effect against normal cell lines even at high concentration, whereas the other set of six compounds (Group A) display a toxic effect. The drug likeliness and pharmacokinetic properties reveal that the compounds can be lead drug materials against breast cancer.
{"title":"Evaluating a series of new curcumin derivatives as potential anti-breast cancer agents: A collective analysis of in-vitro and in-silico characterization","authors":"R. Yuvashri , Era Dravida Thendral , D. Reuben Jonathan , A. Anish Fathima , K. Laavanya , G. Usha","doi":"10.1016/j.chphi.2024.100663","DOIUrl":"https://doi.org/10.1016/j.chphi.2024.100663","url":null,"abstract":"<div><p>In this work, a series of curcumin derivatives have been synthesized using Claisen Schmidt condensation reaction & Schotten-Baumann reaction, and they were screened through in-silico and in-vitro analysis to determine their capacity as a potential agent against breast cancer. Molecular docking reveals that the compounds are in good fit in the active site region of the target protein. Anti-cancer activity reveals that compounds are highly active against the MCF-7 cell lines, even at low concentration. Among the synthesized compounds, a set of five (Group B) exhibits a nontoxic effect against normal cell lines even at high concentration, whereas the other set of six compounds (Group A) display a toxic effect. The drug likeliness and pharmacokinetic properties reveal that the compounds can be lead drug materials against breast cancer.</p></div>","PeriodicalId":9758,"journal":{"name":"Chemical Physics Impact","volume":null,"pages":null},"PeriodicalIF":3.8,"publicationDate":"2024-06-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S266702242400207X/pdfft?md5=59b485f3194f21a797063e7eb7cf1a17&pid=1-s2.0-S266702242400207X-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141482429","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-22DOI: 10.1016/j.chphi.2024.100665
M Sekar , K Saravanan , M Prasath , S Bharathi Bernadsha
In this study,MoS2/g-C3N4Nano flower like composite is synthesizedusing hydrothermal procedure to identify its photo catalytic properties on Methyl Dyes. The morphology, structure and optical properties of the produced materials are studied by X-Ray Diffraction, Fourier Transform Infrared Spectroscopy, FESEM, EDAX and UV –Vis Spectroscopy. The results received through characterizations confirmed that g-C3N4nanosheets are embedded with flower-like MoS2.The construction of the hetero junction is successful and widened absorptionrange in visible light is identified. Iste water contaminated by methyl dyes can be purified using thesynthesized composite. The suitability of the synthesized composite can be efficient in the removal of methyl dyes from industrial istes and domestic istes.
本研究采用水热法合成了 MoS2/g-C3N4 纳米花状复合材料,以确定其对甲基染料的光催化性能。通过 X 射线衍射、傅立叶变换红外光谱、FESEM、EDAX 和紫外可见光谱研究了所制材料的形貌、结构和光学特性。表征结果证实 g-C3N4 纳米片嵌入了花状 MoS2。利用合成的复合材料可以净化被甲基染料污染的废水。合成的复合材料可有效去除工业废水和生活污水中的甲基染料。
{"title":"An investigation on the synthesis and characterization of MoS2 nanoflowers draped g-C3N4 nano sheet (g-C3N4 / MoS2 / MnOOH) ternary composite for the efficient photocatalytic applications","authors":"M Sekar , K Saravanan , M Prasath , S Bharathi Bernadsha","doi":"10.1016/j.chphi.2024.100665","DOIUrl":"https://doi.org/10.1016/j.chphi.2024.100665","url":null,"abstract":"<div><p>In this study,MoS<sub>2</sub>/g-C<sub>3</sub>N<sub>4</sub>Nano flower like composite is synthesizedusing hydrothermal procedure to identify its photo catalytic properties on Methyl Dyes. The morphology, structure and optical properties of the produced materials are studied by X-Ray Diffraction, Fourier Transform Infrared Spectroscopy, FESEM, EDAX and UV –Vis Spectroscopy. The results received through characterizations confirmed that g-C<sub>3</sub>N<sub>4</sub>nanosheets are embedded with flower-like MoS<sub>2</sub>.The construction of the hetero junction is successful and widened absorptionrange in visible light is identified. Iste water contaminated by methyl dyes can be purified using thesynthesized composite. The suitability of the synthesized composite can be efficient in the removal of methyl dyes from industrial istes and domestic istes.</p></div>","PeriodicalId":9758,"journal":{"name":"Chemical Physics Impact","volume":null,"pages":null},"PeriodicalIF":3.8,"publicationDate":"2024-06-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2667022424002093/pdfft?md5=d1cc12ea79c07c81baf027dec8bfc509&pid=1-s2.0-S2667022424002093-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141482428","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-22DOI: 10.1016/j.chphi.2024.100666
Siveswari A, Gowthami V
The current work employs a novel approach to construct a composite nanostructure to improve the capacitive performance of a supercapacitor device. The work involved preparing cube-shaped WO3 particles and depositing them onto the surface of NiCo2O4 needles using a microwave technique. The structure of the composites enables efficient paths for ion transport and electron diffusion in supercapacitors. The hybrid composite electrode demonstrates a specific capacitance of 716 F g−1 at a current density of 5 Ag−1. The asymmetric capacitor device, which utilizes NiCo2O4@WO3 as the positive electrode and AC as the negative electrode, exhibits an energy density of 48.57 Wh kg−1 at a power density of 1120 W kg−1. In addition, the NiCo2O4@WO3//AC device has a favourable cycle life, maintaining 85.7 % of its capacitance retention after 10,000 cycles. The findings demonstrate the potential of NiCo2O4@WO3//AC to be used in the development of advanced hybrid electrodes for improved supercapacitors.
{"title":"Hierarchical NiCo2O4 needle-like heterostructure arrays anchored on WO3 as high- performance asymmetric supercapacitors for energy storage applications","authors":"Siveswari A, Gowthami V","doi":"10.1016/j.chphi.2024.100666","DOIUrl":"https://doi.org/10.1016/j.chphi.2024.100666","url":null,"abstract":"<div><p>The current work employs a novel approach to construct a composite nanostructure to improve the capacitive performance of a supercapacitor device. The work involved preparing cube-shaped WO<sub>3</sub> particles and depositing them onto the surface of NiCo<sub>2</sub>O<sub>4</sub> needles using a microwave technique. The structure of the composites enables efficient paths for ion transport and electron diffusion in supercapacitors. The hybrid composite electrode demonstrates a specific capacitance of 716 F <em>g</em><sup>−1</sup> at a current density of 5 Ag<sup>−1</sup>. The asymmetric capacitor device, which utilizes NiCo<sub>2</sub>O<sub>4</sub>@WO<sub>3</sub> as the positive electrode and AC as the negative electrode, exhibits an energy density of 48.57 Wh kg<sup>−1</sup> at a power density of 1120 W kg<sup>−1</sup>. In addition, the NiCo<sub>2</sub>O<sub>4</sub>@WO<sub>3</sub>//AC device has a favourable cycle life, maintaining 85.7 % of its capacitance retention after 10,000 cycles. The findings demonstrate the potential of NiCo<sub>2</sub>O<sub>4</sub>@WO<sub>3</sub>//AC to be used in the development of advanced hybrid electrodes for improved supercapacitors.</p></div>","PeriodicalId":9758,"journal":{"name":"Chemical Physics Impact","volume":null,"pages":null},"PeriodicalIF":3.8,"publicationDate":"2024-06-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S266702242400210X/pdfft?md5=beb29f1195cec3f1c016132d8080af8d&pid=1-s2.0-S266702242400210X-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141482431","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}