Pub Date : 2024-08-03DOI: 10.1016/j.jcrysgro.2024.127841
Amorphous Ca–Mg carbonate (ACMC) is an important precursor phase of carbonate, and it is of great significance for understanding the process of microbial induced carbonate mineralization and the synthesis of new biomimetic mineral materials. Currently, the biomineralization role of ACMC remains controversial. Therefore, this study conducted experiments on ACMC-induced mineralization under the action of bacteria and their extracellular polymeric substances (EPS). The results show that bacteria and their secretion of EPS contributed to the formation and stability of hydrated Mg-rich ACMC, and affected the polymorphism and morphology of minerals. Bacterial cells and EPS could provide nucleation sites for ACMC precipitation, and they could also be easily adsorbed or encapsulated by ACMC and mineral particles. EPS, Mg2+, or both were conducive to the formation of aqueous amorphous phase, and could stabilize ACMC through surface adsorption and incorporation. The results of this study help to reveal the biomineralization role of ACMC and promote understanding of the formation and transformation process of Ca-Mg carbonate.
{"title":"The roles of amorphous phase on Ca–Mg carbonate mineralization under the action of bacteria and EPS","authors":"","doi":"10.1016/j.jcrysgro.2024.127841","DOIUrl":"10.1016/j.jcrysgro.2024.127841","url":null,"abstract":"<div><p>Amorphous Ca–Mg carbonate (ACMC) is an important precursor phase of carbonate, and it is of great significance for understanding the process of microbial induced carbonate mineralization and the synthesis of new biomimetic mineral materials. Currently, the biomineralization role of ACMC remains controversial. Therefore, this study conducted experiments on ACMC-induced mineralization under the action of bacteria and their extracellular polymeric substances (EPS). The results show that bacteria and their secretion of EPS contributed to the formation and stability of hydrated Mg-rich ACMC, and affected the polymorphism and morphology of minerals. Bacterial cells and EPS could provide nucleation sites for ACMC precipitation, and they could also be easily adsorbed or encapsulated by ACMC and mineral particles. EPS, Mg<sup>2+</sup>, or both were conducive to the formation of aqueous amorphous phase, and could stabilize ACMC through surface adsorption and incorporation. The results of this study help to reveal the biomineralization role of ACMC and promote understanding of the formation and transformation process of Ca-Mg carbonate.</p></div>","PeriodicalId":353,"journal":{"name":"Journal of Crystal Growth","volume":null,"pages":null},"PeriodicalIF":1.7,"publicationDate":"2024-08-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141946100","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-03DOI: 10.1016/j.jcrysgro.2024.127842
Solid solutions based on (Eu,Gd)Sc3(BO3)4 (C2/c) and Gd0.25Sc0.75BO3 (R ) in the EuSc3(BO3)4-GdSc3(BO3)4 system were studied. Synthesis at 1250 °C provides wide homogeneity regions which are stable at room temperature. Melt-solution crystallization of both compounds from LiBO2-LiF flux was shown. All the obtained samples have luminescence characteristic of Eu3+ with a largest peak at 615 nm corresponding to the 5D0 → 7F2 transition. In this series the luminescence intensity monotonically increases with an increase of Eu content. The largest quantum yield of luminescence (53 %) in the EuSc3(BO3)4-GdSc3(BO3)4 system is demonstrated by EuSc3(BO3)4 sample.
{"title":"Solid solutions in EuSc3(BO3)4-GdSc3(BO3)4 system: Phase diagram, synthesis, crystal growth, structure and luminescence","authors":"","doi":"10.1016/j.jcrysgro.2024.127842","DOIUrl":"10.1016/j.jcrysgro.2024.127842","url":null,"abstract":"<div><p>Solid solutions based on (Eu<sub>,</sub>Gd)Sc<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub> (C2/c) and Gd<sub>0.25</sub>Sc<sub>0.75</sub>BO<sub>3</sub> (<em>R</em> <span><math><mrow><mover><mrow><mn>3</mn></mrow><mrow><mo>¯</mo></mrow></mover></mrow></math></span>) in the EuSc<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub>-GdSc<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub> system were studied. Synthesis at 1250 °C provides wide homogeneity regions which are stable at room temperature. Melt-solution crystallization of both compounds from LiBO<sub>2</sub>-LiF flux was shown. All the obtained samples have luminescence characteristic of Eu<sup>3+</sup> with a largest peak at 615 nm corresponding to the <sup>5</sup>D<sub>0</sub> → <sup>7</sup>F<sub>2</sub> transition. In this series the luminescence intensity monotonically increases with an increase of Eu content. The largest quantum yield of luminescence (53 %) in the EuSc<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub>-GdSc<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub> system is demonstrated by EuSc<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub> sample.</p></div>","PeriodicalId":353,"journal":{"name":"Journal of Crystal Growth","volume":null,"pages":null},"PeriodicalIF":1.7,"publicationDate":"2024-08-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141978937","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-02DOI: 10.1016/j.jcrysgro.2024.127839
Bismuth Selenide has gained a great deal of attention as a thermoelectric material owing to its lower toxicity compared to Bi2Te3 based materials. In this work, Sulfur substitution in Bi2Se3 is carried out by the vertical Bridgman method and the influence of Sulfur on the structural, electrical and thermal properties of Bi2Se3 was studied. The thermoelectric figure of merit (ZT) was calculated from electrical conductivity, Seebeck coefficient and thermal conductivity, which were measured from 303 K to 773 K. Sulfur incorporation did not improve the electrical conductivity of Bi2Se3 but proved to be beneficial in improving the Seebeck coefficient and reducing thermal conductivity. Hence, the calculated figure of merit of Bi2Se2.7S0.3 crystal comes out to be 0.72 at 543 K, which is higher than that of pure Bi2Se3 crystal, which is 0.31 at 533 K.
硒化铋作为一种热电材料,因其毒性低于碲化镉(BiTe)材料而备受关注。在这项工作中,采用垂直布里奇曼法在 BiSe 中进行了硫替代,并研究了硫对 BiSe 结构、电学和热学特性的影响。在 303 K 至 773 K 的温度范围内,通过测量电导率、塞贝克系数和热导率计算出了热电功勋值 (ZT)。因此,BiSeS 晶体在 543 K 时的计算值为 0.72,高于纯 BiSe 晶体在 533 K 时的 0.31。
{"title":"Improvement in thermoelectric figure of merit of Bi2Se3 crystal with Sulfur substitution","authors":"","doi":"10.1016/j.jcrysgro.2024.127839","DOIUrl":"10.1016/j.jcrysgro.2024.127839","url":null,"abstract":"<div><p>Bismuth Selenide has gained a great deal of attention as a thermoelectric material owing to its lower toxicity compared to Bi<sub>2</sub>Te<sub>3</sub> based materials. In this work, Sulfur substitution in Bi<sub>2</sub>Se<sub>3</sub> is carried out by the vertical Bridgman method and the influence of Sulfur on the structural, electrical and thermal properties of Bi<sub>2</sub>Se<sub>3</sub> was studied. The thermoelectric figure of merit (ZT) was calculated from electrical conductivity, Seebeck coefficient and thermal conductivity, which were measured from 303 K to 773 K. Sulfur incorporation did not improve the electrical conductivity of Bi<sub>2</sub>Se<sub>3</sub> but proved to be beneficial in improving the Seebeck coefficient and reducing thermal conductivity. Hence, the calculated figure of merit of Bi<sub>2</sub>Se<sub>2.7</sub>S<sub>0.3</sub> crystal comes out to be 0.72 at 543 K, which is higher than that of pure Bi<sub>2</sub>Se<sub>3</sub> crystal, which is 0.31 at 533 K.</p></div>","PeriodicalId":353,"journal":{"name":"Journal of Crystal Growth","volume":null,"pages":null},"PeriodicalIF":1.7,"publicationDate":"2024-08-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141946102","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-02DOI: 10.1016/j.jcrysgro.2024.127836
The present work will systematically study the effect of different linear antenna microwave plasma enhanced chemical vapor deposition (LACVD) processing parameters on the optimal deposition of the diamond films. The low pressure and low temperatures of LACVD growth conditions is expected to deposit diamond films on otherwise reactive gallium nitride (GaN) surfaces, without any intermediate nitride buffer layer. First, the distances between the quartz tube and the samples put on the stage are varied (3–15 cm), which has a direct impact on the substrate temperature (415°–300 °C). Thereafter, the microwave input power was also altered (1.5–2.8 kW) to attain low substrate temperatures. It was found that 300 °C is the temperature limit, which can be attained by heating only with microwave plasma when the substrates are kept farthest (15 cm) away from the liner antenna quartz tube. An additional heater was used under the stage for rapidly achieving such minimum substrate temperature of 300 °C. Substrate heater was used for efficient growth of the diamond phase while using pulse mode frequency of microwave power input for optimization of the diamond films. The microstructure (plate-like and cauliflower-like) of the deposited nanocrystalline diamond (NCD) films and the cross-sectional images for thickness measurements was observed under the scanning electron microscope and the elemental analysis of the film surfaces was done by electron diffraction spectroscopy. Moreover, the diamond film quality and crystallinity were evaluated by Raman spectroscopy with 488 nm laser light. Diamond-on-GaN film results were compared with conventional Si substrate. Different LACVD reactor parameters like, antenna to stage distances, microwave input power in continuous wave mode, and growth temperatures have significant impacts on the grown films, both in terms of their quality and microstructure. It was found that the optimum deposition of nanocrystalline diamond film on GaN substrates without its surface etching was possible, under pulse mode (20 kHz, 45 % duty cycle) with 2 kW average input microwave power.
{"title":"Effect of linear antenna chemical vapor deposition process parameters on the growth of nanocrystalline diamond-on-GaN films","authors":"","doi":"10.1016/j.jcrysgro.2024.127836","DOIUrl":"10.1016/j.jcrysgro.2024.127836","url":null,"abstract":"<div><p>The present work will systematically study the effect of different linear antenna microwave plasma enhanced chemical vapor deposition (LACVD) processing parameters on the optimal deposition of the diamond films. The low pressure and low temperatures of LACVD growth conditions is expected to deposit diamond films on otherwise reactive gallium nitride (GaN) surfaces, without any intermediate nitride buffer layer. First, the distances between the quartz tube and the samples put on the stage are varied (3–15 cm), which has a direct impact on the substrate temperature (415°–300 °C). Thereafter, the microwave input power was also altered (1.5–2.8 kW) to attain low substrate temperatures. It was found that 300 °C is the temperature limit, which can be attained by heating only with microwave plasma when the substrates are kept farthest (15 cm) away from the liner antenna quartz tube. An additional heater was used under the stage for rapidly achieving such minimum substrate temperature of 300 °C. Substrate heater was used for efficient growth of the diamond phase while using pulse mode frequency of microwave power input for optimization of the diamond films. The microstructure (plate-like and cauliflower-like) of the deposited nanocrystalline diamond (NCD) films and the cross-sectional images for thickness measurements was observed under the scanning electron microscope and the elemental analysis of the film surfaces was done by electron diffraction spectroscopy. Moreover, the diamond film quality and crystallinity were evaluated by Raman spectroscopy with 488 nm laser light. Diamond-on-GaN film results were compared with conventional Si substrate. Different LACVD reactor parameters like, antenna to stage distances, microwave input power in continuous wave mode, and growth temperatures have significant impacts on the grown films, both in terms of their quality and microstructure. It was found that the optimum deposition of nanocrystalline diamond film on GaN substrates without its surface etching was possible, under pulse mode (20 kHz, 45 % duty cycle) with 2 kW average input microwave power.</p></div>","PeriodicalId":353,"journal":{"name":"Journal of Crystal Growth","volume":null,"pages":null},"PeriodicalIF":1.7,"publicationDate":"2024-08-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141946103","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-31DOI: 10.1016/j.jcrysgro.2024.127835
This study describes the RF magnetron sputtering growth of nickel (Ni) doped zinc oxide (ZnO) thin films with nanocolumns (NCs) structures. Using a nickel seed layer, homogeneous and vertically aligned ZnO nanocolumns with a diameter of around 30 nm were successfully grown. The X-ray diffraction (XRD) results confirmed the incorporation of Ni atoms into the ZnO lattice, producing single crystalline structures without secondary phases. High-resolution transmission electron microscopy showed clear lattice planes with a d-spacing value of 3.243 Å corresponding to the wurtzite phase of ZnO. Optimal crystalline quality was achieved by growing the films at 300 °C followed by thermal annealing at 300–500 °C in an oxygen ambient.
本研究介绍了射频磁控溅射法生长具有纳米柱(NC)结构的掺杂镍(Ni)氧化锌(ZnO)薄膜。利用镍种子层,成功生长出均匀且垂直排列的氧化锌纳米柱,直径约为 30 纳米。X 射线衍射(XRD)结果证实,镍原子融入了氧化锌晶格,产生了无次生相的单晶结构。高分辨率透射电子显微镜显示出清晰的晶格平面,其 d 间距值为 3.243 Å,对应于氧化锌的钨锌相。薄膜在 300 °C 下生长,然后在氧气环境中进行 300-500 °C 的热退火,从而获得了最佳的结晶质量。
{"title":"Radio frequency magnetron sputtering growth of Ni-doped ZnO thin films with nanocolumnar structures","authors":"","doi":"10.1016/j.jcrysgro.2024.127835","DOIUrl":"10.1016/j.jcrysgro.2024.127835","url":null,"abstract":"<div><p>This study describes the RF magnetron sputtering growth of nickel (Ni) doped zinc oxide (ZnO) thin films with nanocolumns (NCs) structures. Using a nickel seed layer, homogeneous and vertically aligned ZnO nanocolumns with a diameter of around 30 nm were successfully grown. The X-ray diffraction (XRD) results confirmed the incorporation of Ni atoms into the ZnO lattice, producing single crystalline structures without secondary phases. High-resolution transmission electron microscopy showed clear lattice planes with a d-spacing value of 3.243 Å corresponding to the wurtzite phase of ZnO. Optimal crystalline quality was achieved by growing the films at 300 °C followed by thermal annealing at 300–500 °C in an oxygen ambient.</p></div>","PeriodicalId":353,"journal":{"name":"Journal of Crystal Growth","volume":null,"pages":null},"PeriodicalIF":1.7,"publicationDate":"2024-07-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141946105","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-31DOI: 10.1016/j.jcrysgro.2024.127827
The escalating occurrence of antibiotic resistance has focused scientific investigation on the creation of alternative treatments. In this work, an environmentally benign and sustainable method of producing silver nanoparticles (AgNPs) utilizing an aqueous extract from Artocarpus heterophyllus leaves is reported. The study aimed to evaluate the antibacterial and antibiofilm properties of AgNPs against a range of pathogens, specifically Methicillin-resistant Staphylococcus aureus (MRSA), Acinetobacter baumannii, Pseudomonas aeruginosa, and Klebsiella pneumoniae. The antioxidant activity of these AgNPs was also determined.
Methods
The biosynthesis of silver nanoparticles was confirmed and characterized using a range of analytical methods. These methods included UV–visible spectroscopy, Fourier transform infrared (FT-IR) spectroscopy, Laser Particle Sizer, Field emission scanning electron microscopy (FE-SEM), Transmission electron microscopy (TEM), and X-ray diffraction (XRD) analysis. Broth microdilution method was used to assess their antibacterial activity. A free radical scavenging assay was used to determine their antioxidant activity.
Results
At 471 nm in wavelength, the AgNPs’ peak absorbance was measured. The AgNPs had an average size of 97.3 nm. AgNPs were found to have a face-centered cubic structure according to XRD measurements. The EDX analysis represented elemental silver (Ag0) at a concentration of 87.6 %. The synthesized AgNPs possessed antioxidant activity with IC50 value of 35.16 μg/mL. The synthesized nanoparticles demonstrated remarkable antibacterial activity against several bacterial strains, as evidenced by their low minimum inhibitory concentration (MIC) and minimum bactericidal concentration (MBC) values in the ranges of 62.5 to 125 μg/mL. Furthermore, the AgNPs demonstrated potent anti-biofilm properties, significantly decreasing the formation of biofilms. In addition to these promising antimicrobials, antibiofilm and antioxidant properties.
Conclusions
The results of this study indicate that the environmentally friendly AgNPs that were synthesized have considerable potential as antibacterial and antibiofilm agents; they provide a sustainable substitute for addressing the issue of antibiotic resistance. Their possible application in clinical settings calls for further thorough research.
{"title":"Biofabrication of silver nanoparticles using Artocarpus heterophyllus leaves extract: Characterization and evaluation of its antibacterial, antibiofilm, and antioxidant activities","authors":"","doi":"10.1016/j.jcrysgro.2024.127827","DOIUrl":"10.1016/j.jcrysgro.2024.127827","url":null,"abstract":"<div><p>The escalating occurrence of antibiotic resistance has focused scientific investigation on the creation of alternative treatments. In this work, an environmentally benign and sustainable method of producing silver nanoparticles (AgNPs) utilizing an aqueous extract from <em>Artocarpus heterophyllus</em> leaves is reported. The study aimed to evaluate the antibacterial and antibiofilm properties of AgNPs against a range of pathogens, specifically Methicillin-resistant <em>Staphylococcus aureus</em> (MRSA), <em>Acinetobacter baumannii</em>, <em>Pseudomonas aeruginosa</em>, and <em>Klebsiella pneumoniae</em>. The antioxidant activity of these AgNPs was also determined.</p></div><div><h3>Methods</h3><p>The biosynthesis of silver nanoparticles was confirmed and characterized using a range of analytical methods. These methods included UV–visible spectroscopy, Fourier transform infrared (FT-IR) spectroscopy, Laser Particle Sizer, Field emission scanning electron microscopy (FE-SEM), Transmission electron microscopy (TEM), and X-ray diffraction (XRD) analysis. Broth microdilution method was used to assess their antibacterial activity. A free radical scavenging assay was used to determine their antioxidant activity.</p></div><div><h3>Results</h3><p>At 471 nm in wavelength, the AgNPs’ peak absorbance was measured. The AgNPs had an average size of 97.3 nm. AgNPs were found to have a face-centered cubic structure according to XRD measurements. The EDX analysis represented elemental silver (Ag<sup>0</sup>) at a concentration of 87.6 %. The synthesized AgNPs possessed antioxidant activity with IC<sub>50</sub> value of 35.16 μg/mL. The synthesized nanoparticles demonstrated remarkable antibacterial activity against several bacterial strains, as evidenced by their low minimum inhibitory concentration (MIC) and minimum bactericidal concentration (MBC) values in the ranges of 62.5 to 125 μg/mL. Furthermore, the AgNPs demonstrated potent anti-biofilm properties, significantly decreasing the formation of biofilms. In addition to these promising antimicrobials, antibiofilm and antioxidant properties.</p></div><div><h3>Conclusions</h3><p>The results of this study indicate that the environmentally friendly AgNPs that were synthesized have considerable potential as antibacterial and antibiofilm agents; they provide a sustainable substitute for addressing the issue of antibiotic resistance. Their possible application in clinical settings calls for further thorough research.</p></div>","PeriodicalId":353,"journal":{"name":"Journal of Crystal Growth","volume":null,"pages":null},"PeriodicalIF":1.7,"publicationDate":"2024-07-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141946106","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-31DOI: 10.1016/j.jcrysgro.2024.127837
Single crystals of a novel silver borate nitrate, Ag12(B9O18)(NO3)3 (1), were produced as a byproduct upon preparation of Ag3B6O10(NO3). 1 is hexagonal, (P63/m, a = 11.2896(3) Å, c = 11.6693(3) Å); its structure exhibits just a second example of unique [B9O18]9– nonaborate anions [9B:6Δ3□:3(<2Δ□>–)<3□>] which can be described as three triborate groups linked in a large cycle. As commonly observed among silver borates, the Ag+ cations exhibit strongly anharmonic vibrations which were described using Gram–Chariler series up to 4th order. 1 is characterized by single-crystal X-ray diffraction, variable-temperature powder X-ray diffraction, IR, Raman, and UV–vis-NIR spectroscopy, complex thermal analysis, and DFT calculations. The thermal expansion of 1 is slightly anisotropic (αa = 15.0, αc = 17.7 × 10−6 °C−1 at 200 °C). Upon heating, the compound decomposes with formation of metallic silver and another borate, AgBO2, which could be earlier prepared only at high oxygen pressure.
新型硝酸银硼酸盐 Ag(BO)(NO) ()的单晶是在制备 AgBO(NO) 时产生的副产品,呈六边形 (6/, = 11.2896(3) Å, = 11.6693(3) Å);其结构显示了独特的[BO]非硼酸盐阴离子[9B:6Δ3□:3(-)]的第二个例子,可描述为三个三硼酸盐基团连接在一个大循环中。通过单晶 X 射线衍射、变温粉末 X 射线衍射、红外光谱、拉曼光谱、紫外-可见-近红外光谱、复合热分析和 DFT 计算,我们发现硼酸银的阳离子表现出强烈的非谐振动。该化合物的热膨胀略呈各向异性(200 °C 时 = 15.0, = 17.7 × 10 °C)。加热时,化合物分解,形成金属银和另一种硼酸盐 AgBO。
{"title":"The further development of the borate nitrate family: Synthesis and characterization of Ag12(B9O18)(NO3)3 with unique isolated B9O18 clusters, 9B:6Δ3□:3(<2Δ□>–)<3□>","authors":"","doi":"10.1016/j.jcrysgro.2024.127837","DOIUrl":"10.1016/j.jcrysgro.2024.127837","url":null,"abstract":"<div><p>Single crystals of a novel silver borate nitrate, Ag<sub>12</sub>(B<sub>9</sub>O<sub>18</sub>)(NO<sub>3</sub>)<sub>3</sub> (<strong>1</strong>), were produced as a byproduct upon preparation of Ag<sub>3</sub>B<sub>6</sub>O<sub>10</sub>(NO<sub>3</sub>). <strong>1</strong> is hexagonal, (<em>P</em>6<sub>3</sub>/<em>m</em>, <em>a</em> = 11.2896(3) Å, <em>c</em> = 11.6693(3) Å); its structure exhibits just a second example of unique [B<sub>9</sub>O<sub>18</sub>]<sup>9–</sup> nonaborate anions [9B:6Δ3□:3(<2Δ□>–)<3□>] which can be described as three triborate groups linked in a large cycle. As commonly observed among silver borates, the Ag<sup>+</sup> cations exhibit strongly anharmonic vibrations which were described using Gram–Chariler series up to 4th order. <strong>1</strong> is characterized by single-crystal X-ray diffraction, variable-temperature powder X-ray diffraction, IR, Raman, and UV–vis-NIR spectroscopy, complex thermal analysis, and DFT calculations. The thermal expansion of <strong>1</strong> is slightly anisotropic (<em>α<sub>a</sub></em> = 15.0, <em>α</em><sub>c</sub> = 17.7 × 10<sup>−6</sup> °C<sup>−1</sup> at 200 °C). Upon heating, the compound decomposes with formation of metallic silver and another borate, AgBO<sub>2</sub>, which could be earlier prepared only at high oxygen pressure.</p></div>","PeriodicalId":353,"journal":{"name":"Journal of Crystal Growth","volume":null,"pages":null},"PeriodicalIF":1.7,"publicationDate":"2024-07-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141946104","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-28DOI: 10.1016/j.jcrysgro.2024.127823
The cross-point (Cp), which appears in the vacancy (CV) and interstitial Si atom (CI) concentration curves, is a simple controlling factor for ingot growth and provides a final goal to obtain a defect-free Si ingot using general Si melt growth. The importance of Cp is demonstrated using the noncontact crucible method (NOC), which has a relatively small temperature gradient due to an ingot grown inside the melt. The control of temperature gradient G at a constant growth rate v is simple for the actual ingot growth; thus, the present simulated results are expressed by G at a constant v. The concentration at the Cp point becomes smaller as G becomes smaller and finally becomes zero (Cp = 0), in which CV and CI are practically zero (CV=CI=0). The estimated G and temperature T at Cp = 0 for v = 0.000144 cm s−1 are 6.3, 12.5, and 18.5 K cm−1 and 1216 K (943 °C), 1354 K (1081 °C), and 1371 K (1098 °C), corresponding to each combination. At 1216 K, G should be precisely controlled within 6.3 ± 3 % K cm−1 in the region substantially close to Cp = 0 to maintain the remaining concentration of point defects substantially lower than 1.0 × 1013 cm−3. G should be changed during growth from larger G to smaller G, such as 6.3 K cm−1, to efficiently grow the ingot within the limited time. The changing point, x of G, is an important key parameter for the timing variation, where x denotes the normalized distance from the growing interface. The initial G is large; thus, the changing point of G approaches the growing interface. The growth condition necessary to obtain a defect-free Si ingot can be demonstrated using the Cp = 0 point, which is fully compatible with the perfect critical point where CV and CI are practically zero. The present results are mainly considered using the CV and CI concentration curves. However, these results largely help understand the approximate trend of G and v for the growth of defect-free ingot and the relation between Cp and the commonly used critical point between CV and CI.
出现在空位(CV)和间隙硅原子(CI)浓度曲线中的交叉点(Cp)是硅锭生长的一个简单控制因素,也是利用一般硅熔体生长获得无缺陷硅锭的最终目标。使用非接触坩埚法(NOC)证明了 Cp 的重要性,由于硅锭生长在熔体内部,因此温度梯度相对较小。Cp 点的浓度随着 G 的变小而变小,最后变为零(Cp = 0),此时 CV 和 CI 实际上为零(CV=CI=0)。在 v = 0.000144 cm s-1 条件下,Cp = 0 时的 G 和温度 T 分别为 6.3、12.5 和 18.5 K cm-1 以及 1216 K(943 °C)、1354 K(1081 °C)和 1371 K(1098 °C)。在 1216 K 时,G 值应精确控制在 6.3 ± 3 % K cm-1 的范围内,即基本接近 Cp = 0 的区域,以保持剩余的点缺陷浓度大大低于 1.0 × 1013 cm-3。在生长过程中,应将 G 从较大的 G 变为较小的 G,如 6.3 K cm-1,以便在有限的时间内有效地生长铸锭。G 的变化点 x 是时间变化的重要关键参数,其中 x 表示与生长界面的归一化距离。初始 G 较大,因此 G 的变化点接近生长界面。获得无缺陷硅锭所需的生长条件可以用 Cp = 0 点来证明,该点完全符合完美临界点,即 CV 和 CI 几乎为零。目前的结果主要是通过 CV 和 CI 浓度曲线来考虑的。然而,这些结果在很大程度上有助于理解无缺陷硅锭生长过程中 G 和 v 的大致趋势,以及 Cp 与常用的 CV 和 CI 临界点之间的关系。
{"title":"Importance of zero cross-point (Cp = 0) control between the vacancy and interstitial Si atom concentration curves to obtain a perfect Si ingot using Si melt growth","authors":"","doi":"10.1016/j.jcrysgro.2024.127823","DOIUrl":"10.1016/j.jcrysgro.2024.127823","url":null,"abstract":"<div><p>The cross-point (Cp), which appears in the vacancy (<em>C<sub>V</sub></em>) and interstitial Si atom (<em>C<sub>I</sub></em>) concentration curves, is a simple controlling factor for ingot growth and provides a final goal to obtain a defect-free Si ingot using general Si melt growth. The importance of Cp is demonstrated using the noncontact crucible method (NOC), which has a relatively small temperature gradient due to an ingot grown inside the melt. The control of temperature gradient <em>G</em> at a constant growth rate <em>v</em> is simple for the actual ingot growth; thus, the present simulated results are expressed by <em>G</em> at a constant <em>v</em>. The concentration at the Cp point becomes smaller as <em>G</em> becomes smaller and finally becomes zero (Cp = 0), in which <em>C<sub>V</sub></em> and <em>C<sub>I</sub></em> are practically zero (<em>C<sub>V</sub></em>=<em>C<sub>I</sub></em>=0). The estimated <em>G</em> and temperature <em>T</em> at Cp = 0 for <em>v</em> = 0.000144 cm s<sup>−1</sup> are 6.3, 12.5, and 18.5 K cm<sup>−1</sup> and 1216 K (943 °C), 1354 K (1081 °C), and 1371 K (1098 °C), corresponding to each combination. At 1216 K, <em>G</em> should be precisely controlled within 6.3 ± 3 % K cm<sup>−1</sup> in the region substantially close to Cp = 0 to maintain the remaining concentration of point defects substantially lower than 1.0 × 10<sup>13</sup> cm<sup>−3</sup>. <em>G</em> should be changed during growth from larger <em>G</em> to smaller <em>G</em>, such as 6.3 K cm<sup>−1</sup>, to efficiently grow the ingot within the limited time. The changing point, <em>x</em> of <em>G</em>, is an important key parameter for the timing variation, where <em>x</em> denotes the normalized distance from the growing interface. The initial <em>G</em> is large; thus, the changing point of <em>G</em> approaches the growing interface. The growth condition necessary to obtain a defect-free Si ingot can be demonstrated using the Cp = 0 point, which is fully compatible with the perfect critical point where <em>C<sub>V</sub></em> and <em>C<sub>I</sub></em> are practically zero. The present results are mainly considered using the <em>C<sub>V</sub></em> and <em>C<sub>I</sub></em> concentration curves. However, these results largely help understand the approximate trend of <em>G</em> and <em>v</em> for the growth of defect-free ingot and the relation between Cp and the commonly used critical point between <em>C<sub>V</sub></em> and <em>C<sub>I</sub></em>.</p></div>","PeriodicalId":353,"journal":{"name":"Journal of Crystal Growth","volume":null,"pages":null},"PeriodicalIF":1.7,"publicationDate":"2024-07-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141846854","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-27DOI: 10.1016/j.jcrysgro.2024.127834
This study presents the controlled growth of 3-Mercaptopropionic acid (MPA)-capped ZnS quantum dots (QDs) using a concentration-modulated single injection hydrothermal method. Employing the Concentration optimization by optical spectra (COOS) method, we optimized the MPA:Zn:S ratios to investigate the influence of the capping agent, cation, and anion for exceptional properties suitable for optoelectronic and sensor applications. CMSIH operates as a single-step synthesis process, reducing processing time and complexity. This streamlined approach not only enhances efficiency but also minimizes the risk of contamination and ensures batch-to-batch consistency in QD production. Its moderate operating conditions, compared to other high-energy methods, also contribute to reduced energy consumption and environmental impact, aligning with sustainable manufacturing practices. Further, X-ray diffraction (XRD) confirmed the Zinc blend (cubic) phase of ZnS, and Fourier-transform infrared spectroscopy (FTIR) validated MPA capping. The QDs exhibited strong quantum confinement, causing a blue shift in absorption peaks compared to bulk ZnS. Higher MPA concentrations ranging from 0.02 M to 0.1 M induced a red shift in the absorption edge due to prolonged reaction times and strong cation binding by MPA. Variations in cation Zn and anion S ratios from 0.02 M to 0.1 M caused blue and red shifts in the absorption edge, respectively. For instance, Zn:S = 0.04:0.01 M increased cation concentrations, reducing QD size up to 0.67 nm, while enhanced anion concentrations Zn:S = 0.04:0.04 M enlarged the QDs size up to 2.35 nm. Remarkably, calculated QD sizes using Brus’ equation were smaller than the Bohr radius, even at an elevated temperature of 95 °C, indicating significant quantum confinement. Luminescence studies revealed reduced luminescence with higher MPA concentrations, increased luminescence intensity with higher cation Zn+ concentrations, and a red shift in the luminescence peak with higher anion S concentrations. As the temperature rises, there is an observable decrease in luminescence intensity. Furthermore, the investigation into the relationship between chemical composition and optical properties of MPA-capped ZnS QDs at elevated temperatures expands understanding of quantum confinement effects. The synthesised unique ultra small ZnS QDs can be used in advanced quantum sensors mainly as radiation detectors.
本研究介绍了利用浓度调制单次注入水热法控制 3-巯基丙酸(MPA)封端 ZnS 量子点(QDs)的生长。利用光学光谱浓度优化(COOS)方法,我们优化了 MPA:Zn:S 的比例,研究了封端剂、阳离子和阴离子对适合光电和传感器应用的特殊性能的影响。CMSIH 采用单步合成工艺,缩短了处理时间,降低了复杂性。这种简化方法不仅提高了效率,还最大限度地降低了污染风险,并确保了 QD 生产中批次间的一致性。与其他高能量方法相比,它的操作条件适中,也有助于降低能耗和对环境的影响,符合可持续生产实践。此外,X 射线衍射 (XRD) 证实了 ZnS 的锌混合(立方)相,傅立叶变换红外光谱 (FTIR) 验证了 MPA 封装。与块状 ZnS 相比,QDs 表现出强烈的量子约束,导致吸收峰出现蓝移。由于反应时间延长以及 MPA 与阳离子的强结合,浓度从 0.02 M 到 0.1 M 的较高 MPA 引发了吸收边缘的红移。阳离子 Zn 和阴离子 S 的比例从 0.02 M 到 0.1 M 的变化分别导致吸收边缘发生蓝移和红移。例如,Zn:S = 0.04:0.01 M 增加了阳离子浓度,使 QD 尺寸减小到 0.67 nm,而 Zn:S = 0.04:0.04 M 增加了阴离子浓度,使 QD 尺寸增大到 2.35 nm。值得注意的是,即使在 95 ℃ 的高温条件下,利用布鲁斯方程计算出的 QD 尺寸也小于玻尔半径,这表明量子束缚效果显著。发光研究表明,MPA 浓度越高,发光强度越低;阳离子 Zn+ 浓度越高,发光强度越高;阴离子 S 浓度越高,发光峰越红移。随着温度的升高,发光强度明显下降。此外,对 MPA 封装的 ZnS QDs 在高温下的化学成分和光学特性之间关系的研究,拓展了对量子约束效应的理解。合成的独特超小型 ZnS QDs 可用于先进的量子传感器,主要用作辐射探测器。
{"title":"Controlled growth of MPA-capped ZnS quantum dots through concentration-modulated single injection hydrothermal method","authors":"","doi":"10.1016/j.jcrysgro.2024.127834","DOIUrl":"10.1016/j.jcrysgro.2024.127834","url":null,"abstract":"<div><p>This study presents the controlled growth of 3-Mercaptopropionic acid (MPA)-capped ZnS quantum dots (QDs) using a concentration-modulated single injection hydrothermal method. Employing the Concentration optimization by optical spectra (COOS) method, we optimized the MPA:Zn:S ratios to investigate the influence of the capping agent, cation, and anion for exceptional properties suitable for optoelectronic and sensor applications. CMSIH operates as a single-step synthesis process, reducing processing time and complexity. This streamlined approach not only enhances efficiency but also minimizes the risk of contamination and ensures batch-to-batch consistency in QD production. Its moderate operating conditions, compared to other high-energy methods, also contribute to reduced energy consumption and environmental impact, aligning with sustainable manufacturing practices. Further, X-ray diffraction (XRD) confirmed the Zinc blend (cubic) phase of ZnS, and Fourier-transform infrared spectroscopy (FTIR) validated MPA capping. The QDs exhibited strong quantum confinement, causing a blue shift in absorption peaks compared to bulk ZnS. Higher MPA concentrations ranging from 0.02 M to 0.1 M induced a red shift in the absorption edge due to prolonged reaction times and strong cation binding by MPA. Variations in cation Zn and anion S ratios from 0.02 M to 0.1 M caused blue and red shifts in the absorption edge, respectively. For instance, Zn:S = 0.04:0.01 M increased cation concentrations, reducing QD size up to 0.67 nm, while enhanced anion concentrations Zn:S = 0.04:0.04 M enlarged the QDs size up to 2.35 nm. Remarkably, calculated QD sizes using Brus’ equation were smaller than the Bohr radius, even at an elevated temperature of 95 °C, indicating significant quantum confinement. Luminescence studies revealed reduced luminescence with higher MPA concentrations, increased luminescence intensity with higher cation Zn+ concentrations, and a red shift in the luminescence peak with higher anion S concentrations. As the temperature rises, there is an observable decrease in luminescence intensity. Furthermore, the investigation into the relationship between chemical composition and optical properties of MPA-capped ZnS QDs at elevated temperatures expands understanding of quantum confinement effects. The synthesised unique ultra small ZnS QDs can be used in advanced quantum sensors mainly as radiation detectors.</p></div>","PeriodicalId":353,"journal":{"name":"Journal of Crystal Growth","volume":null,"pages":null},"PeriodicalIF":1.7,"publicationDate":"2024-07-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141850465","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-26DOI: 10.1016/j.jcrysgro.2024.127826
La3Ga5.5Nb0.5O14 (LGN) crystal is a promising material for optical parametric chirped-pulse amplification (OPCPA) with high laser damage threshold and wide transmission range which is able to achieve high peak power laser. LGN with a diameter of 25 mm was successfully grown by the vertical Bridgman method for the first time and a series of characterizations were performed. The 1.7 µm absorption peak in transmittance spectra of LGN crystal which was caused by the Czochralski technique can be effectively eliminated by the vertical Bridgman method. LGN crystal possesses a high transmittance of 81.3 % in the range of 0.294 ∼ 7.500 μm. The experimental optical band gap of LGN is 4.16 eV which is positively correlated with laser damage threshold. The experimental laser damage threshold of LGN was determined to 1.416 GW/cm2 by Nd:YAG. The outstanding thermal properties of LGN indicate that it possesses thermal stability in high energy laser field. This work demonstrates that LGN crystal holds great potential for OPCPA applications and the vertical Bridgman method is proved to be a effective and excellent technique to grow high quality LGN crystal.
{"title":"Bridgman growth and characterizations of nonlinear optical crystal La3Ga5.5Nb0.5O14","authors":"","doi":"10.1016/j.jcrysgro.2024.127826","DOIUrl":"10.1016/j.jcrysgro.2024.127826","url":null,"abstract":"<div><p>La<sub>3</sub>Ga<sub>5.5</sub>Nb<sub>0.5</sub>O<sub>14</sub> (LGN) crystal is a promising material for optical parametric chirped-pulse amplification (OPCPA) with high laser damage threshold and wide transmission range which is able to achieve high peak power laser. LGN with a diameter of 25 mm was successfully grown by the vertical Bridgman method for the first time and a series of characterizations were performed. The 1.7 µm absorption peak in transmittance spectra of LGN crystal which was caused by the Czochralski technique can be effectively eliminated by the vertical Bridgman method. LGN crystal possesses a high transmittance of 81.3 % in the range of 0.294 ∼ 7.500 μm. The experimental optical band gap of LGN is 4.16 eV which is positively correlated with laser damage threshold. The experimental laser damage threshold of LGN was determined to 1.416 GW/cm<sup>2</sup> by Nd:YAG. The outstanding thermal properties of LGN indicate that it possesses thermal stability in high energy laser field. This work demonstrates that LGN crystal holds great potential for OPCPA applications and the vertical Bridgman method is proved to be a effective and excellent technique to grow high quality LGN crystal.</p></div>","PeriodicalId":353,"journal":{"name":"Journal of Crystal Growth","volume":null,"pages":null},"PeriodicalIF":1.7,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141841033","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}