Academic literature on the topic 'Hexagonal crystal structure'

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Journal articles on the topic "Hexagonal crystal structure"

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Brumberg, Alexandra, Kevin Hammonds, Ian Baker, et al. "Single-crystal Ih ice surfaces unveil connection between macroscopic and molecular structure." Proceedings of the National Academy of Sciences 114, no. 21 (2017): 5349–54. http://dx.doi.org/10.1073/pnas.1703056114.

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Physics and chemistry of ice surfaces are not only of fundamental interest but also have important impacts on biological and environmental processes. As ice surfaces—particularly the two prism faces—come under greater scrutiny, it is increasingly important to connect the macroscopic faces with the molecular-level structure. The microscopic structure of the ubiquitous ice Ih crystal is well-known. It consists of stacked layers of chair-form hexagonal rings referred to as molecular hexagons. Crystallographic unit cells can be assembled into a regular right hexagonal prism. The bases are labeled crystallographic hexagons. The two hexagons are rotated 30° with respect to each other. The linkage between the familiar macroscopic shape of hexagonal snowflakes and either hexagon is not obvious per se. This report presents experimental data directly connecting the macroscopic shape of ice crystals and the microscopic hexagons. Large ice single crystals were used to fabricate samples with the basal, primary prism, or secondary prism faces exposed at the surface. In each case, the same sample was used to capture both a macroscopic etch pit image and an electron backscatter diffraction (EBSD) orientation density function (ODF) plot. Direct comparison of the etch pit image and the ODF plot compellingly connects the macroscopic etch pit hexagonal profile to the crystallographic hexagon. The most stable face at the ice–water interface is the smallest area face at the ice–vapor interface. A model based on the molecular structure of the prism faces accounts for this switch.
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Murray, Benjamin J., Christoph G. Salzmann, Andrew J. Heymsfield, Steven Dobbie, Ryan R. Neely, and Christopher J. Cox. "Trigonal Ice Crystals in Earth’s Atmosphere." Bulletin of the American Meteorological Society 96, no. 9 (2015): 1519–31. http://dx.doi.org/10.1175/bams-d-13-00128.1.

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Abstract We are all familiar with the hexagonal shape of snow and ice crystals, and it is well established that their sixfold symmetry is derived from the arrangement of water molecules in a hexagonal crystal structure. However, atmospheric ice crystals with only threefold rotational symmetry are often observed, which is inconsistent with the hexagonal crystal structure of ordinary ice. These crystals are found in a wide range of different cloud types ranging from upper-tropospheric cirrus to contrails and diamond dust and they form at temperatures ranging from about −84° to −5°C. Recent experimental studies of ice crystal structures have shown that ice under a wide range of atmospheric conditions does not always conform to the standard hexagonal crystal structure. Instead, sequences of the hexagonal structure can be interlaced with cubic sequences to create stacking-disordered ice. This degrades the symmetry of the crystal structure so that, instead of having a hexagonal structure, they have a trigonal structure with a corresponding threefold symmetry. Hence, this implies that atmospheric ice crystals with threefold symmetry are made of stacking-disordered ice. We conclude that the presence of trigonal crystals in the atmosphere is consistent with rare Parry arc halos and also show that they have distinct radiative properties compared with hexagonal ice.
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Lee, Geun-Hyoung. "Octahedral-Shaped Zn<sub>2</sub>SnO<sub>4</sub> and Hexagonal Cylinder-like ZnO Crystals Grown via Thermal Evaporation of Mixtures of ZnS and SnO Powders." Korean Journal of Metals and Materials 62, no. 9 (2024): 721–25. http://dx.doi.org/10.3365/kjmm.2024.62.9.721.

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Octahedron-shaped zinc stannate (Zn&lt;sub&gt;2&lt;/sub&gt;SnO&lt;sub&gt;4&lt;/sub&gt;) crystals and hexagonal cylinder-like ZnO crystals were synthesized through a simple thermal evaporation method under uncomplicated conditions of air atmosphere. The Zn&lt;sub&gt;2&lt;/sub&gt;SnO&lt;sub&gt;4&lt;/sub&gt; octahedrons were grown by heating a mixture of ZnS and SnO powders, and the ZnO hexagonal cylinder-like crystals were fabricated by heating mixtures of ZnS, SnO and graphite powders. X-ray diffraction analysis confirmed that the Zn&lt;sub&gt;2&lt;/sub&gt;SnO&lt;sub&gt;4&lt;/sub&gt; crystals had a cubic inverse spinel crystal structure, and the ZnO crystals had a hexagonal wurtzite crystal structure. Scanning electron microscopy analysis revealed that the Zn&lt;sub&gt;2&lt;/sub&gt;SnO&lt;sub&gt;4&lt;/sub&gt; octahedrons had six vertices and eight equilateral triangular faces with very smooth surfaces, and the ZnO crystals had two parallel hexagonal bases and six side faces. Judging from the crystal structure of Zn&lt;sub&gt;2&lt;/sub&gt;SnO&lt;sub&gt;4&lt;/sub&gt;, the octahedral crystals were covered with eight {111} planes. Considering the crystal structure of ZnO, the hexagonal cylinder-like crystals were enclosed by two {001} basal planes and six {100} side planes, which indicated that the ZnO crystals were grown along the [001] direction. When the amount of graphite in the source powder was increased, the aspect ratio of the hexagonal cylinder-like ZnO crystals increased. Energy dispersive x-ray spectroscopy analysis also showed that the octahedral crystals were Zn&lt;sub&gt;2&lt;/sub&gt;SnO&lt;sub&gt;4&lt;/sub&gt;, and the hexagonal cylinder-like crystals were ZnO.
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Iwanaga, Hiroshi, Takeshi Hashishin, Seiji Motojima, Masaki Ichihara, and Shin Takeuchi. "Polymorphism in ZrP crystal." Journal of Materials Research 18, no. 3 (2003): 567–70. http://dx.doi.org/10.1557/jmr.2003.0073.

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Electron microscopy observations of α–ZrP whiskers with the NaCl structure, grown by chemical vapor deposition at 1300 °C, showed that there exists a hexagonal structure region (a = 0.369 nm and c = 1.248 nm) near the surface of the whiskers. High-resolution lattice image observations revealed that the method of stacking the eight-layered hexagonal structure is different from the reported hexagonal β–ZrP. In addition to the eight-layered structure, 12-layered and 16-layered structures were also observed, indicating a variety of ZrP polymorphisms.
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Xin, Haoran, and Tong Cui. "Prediction of Electric Load Neural Network Prediction Model for Big Data." Highlights in Science, Engineering and Technology 104 (June 11, 2024): 155–60. http://dx.doi.org/10.54097/pazjy196.

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In this study, the two-dimensional hexagonal Photonic crystal energy band structure was simulated using COMSOL Multiphysics field simulation software. The 2D hexagonal Photonic crystal structure was constructed by setting parameters such as periodic boundary conditions and air hole radius. Using the frequency domain solver of COMSOL software, the transmission and reflection spectra of the structure were calculated, and the energy band structure diagram was obtained. The effects of different parameters on the energy band structure were analyzed by adjusting the structure parameters. The results show that the fine tuning of the energy band structure of 2D hexagonal Photonic crystals can be realized by adjusting the radius of air holes and the periodic boundary conditions. This study provides a useful reference for further research on the properties and applications of 2D photonic crystals.
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Ayer, Raghavan, J. C. Scanlon, T. A. Ramanarayanan, R. R. Mueller, R. Petkovic-Luton, and J. W. Steeds. "Crystal structure of intermetallic phase in Fe–20Cr–4Al–0.5Y alloy by convergent beam electron diffraction." Journal of Materials Research 2, no. 1 (1987): 16–27. http://dx.doi.org/10.1557/jmr.1987.0016.

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The crystal structure and chemical composition of the intermetallic phase in a Fe-20%Cr-4%Al-0.5%Y (wt. %) alloy were investigated by electron microscopy. Convergent beam diffraction studies revealed that the intermetallic phase forms in three different crystal structures that could coexist in a single grain of the phase. The dominant crystal structure was shown to be hexagonal (a = 0.85, c = 0.84 nm) with a space group most likely to be P63/mmc. Within the hexagonal phase, regions of a rhombohedral crystal structure (a = 0.85, c = 1.26 nm) were observed that had grown in without an apparent phase boundary separating the two crystal structures. The third crystal structure was determined to be monoclinic (a = 0.97, b = 0.85, c = 1.07 nm, and beta = 97.3°) and formed by twinning on the {10$\overline 1$1} planes of the hexagonal phase. The chemical compositions of regions with different crystal structures were comparable and the stoichiometry of the intermetallic phase corresponds to (Fe,Cr)17 (Al,Y)2. The relationship of the observed crystal structures to those previously reported is discussed.
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Pauling, L. "Crystal structure of hexagonal MnAl4." Proceedings of the National Academy of Sciences 84, no. 11 (1987): 3537–39. http://dx.doi.org/10.1073/pnas.84.11.3537.

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Auniq, Reedwan Bin Zafar, Weerapong Lerdrattranataywee, and Upsorn Boonyang. "Microstructural Investigation of Fluoroapatite Hydrothermally Converted from Hydroxyapatite Synthesized from Crocodile Eggshell." Journal of Metastable and Nanocrystalline Materials 32 (April 2021): 21–32. http://dx.doi.org/10.4028/www.scientific.net/jmnm.32.21.

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Fluoro/hydroxyapatite (FHAp) were prepared by hydrothermal at 150 °C for 24 hours with different of starting materials. The conversion of hydroxyapatite (HAp) and tricalcium phosphate to FHAp showed the rod-like shape with 200 nm. While, the morphology of FHAp from crocodile eggshell as CaCO3 form with different in phosphorus and fluoride source showed the unique structure evolution from rod-like hexagonal crystals, dumbbell to ball shape. Two distinctive morphology, first when using NaF as fluoride source with (NH4)2HPO4 precursor show the large cubic structure in high magnification it is tufted hexagonal crystal and it bundle like structure. As the pH value decreases in NH4F, it increases crystal size. For H3PO4 as phosphate precursor found that unique structure evolution from rod-like hexagonal crystals to dumbbell structure and then form the sphere assembly with a size of several micrometers.
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Albrecht, Ralf, Heinrich Menning, Thomas Doert, and Michael Ruck. "Hydroflux synthesis and crystal structure of Tl3IO." Acta Crystallographica Section E Crystallographic Communications 76, no. 10 (2020): 1638–40. http://dx.doi.org/10.1107/s2056989020012359.

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Single-crystals of thallium(I) iodide oxide Tl3IO were obtained as by-product in a hydroflux synthesis at 473 K for 10 h. A potassium hydroxide hydroflux with a water-base molar ratio of 1.6 and the starting materials TlNO3, RhI3 and Ba(NO3)2 was used, resulting in a few black needle-shaped crystals. X-ray diffraction on a single-crystal revealed the hexagonal space group P63/mmc (No. 194) with lattice parameters a = 7.1512 (3) Å and c = 6.3639 (3) Å. Tl3IO crystallizes as hexagonal anti-perovskite (anti-BaNiO3 type) and is thus structurally related to the alkali-metal halide/auride oxides M 3 XO (M = K, Rb, Cs; X = Cl, Br, I, Au). The oxygen atoms center thallium octahedra. The [OTl6] octahedra share trans faces, forming a linear chain along [001]. Twelve thallium atoms surround each iodine atom in an [ITl12] anti-cuboctahedron. Thallium and iodine atoms together form a hexagonal close-sphere packing, in which every fourth octahedral void is occupied by oxygen.
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Zhao, Shanrong, Jin Tan, Jiyang Wang, Xiaobo Hu, and Hong Liu. "Triangular dendrites of LiAlSiO4–SiO2: evolution between threefold- and sixfold-symmetric morphologies." Journal of Applied Crystallography 35, no. 4 (2002): 455–58. http://dx.doi.org/10.1107/s0021889802008038.

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A special kind of triangular dendrite of LiAlSiO4–SiO2(or Li1−xAl1−xSi1+xO4, 0 ≤x≤ 1) in matt glaze has been observed by DIC (differential interference contrast) microscopy. This triangular dendrite is β-quartz with a sixfold-symmetric structure. For polyhedral crystals, a crystal with threefold-symmetric structure prefers to develop a hexagonal prismatic habit rather than a trigonal prismatic habit, because a trigonal prism has a higher surface energy than a hexagonal prism. However, for dendritic crystals, a special kind of triangular dendrite, with a pattern formed by the aggregation of many small triangles, can develop. As supercooling decreases, β-quartz can develop a series of morphologies with different surface energies, from snowflake-shaped dendrite to triangular dendrite, and finally to a polyhedral crystal in the form of a hexagonal prism. This series of crystal morphologies shows a morphological evolution from dendrite to polyhedral crystal, and also shows a morphological evolution between sixfold and threefold symmetries.
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Dissertations / Theses on the topic "Hexagonal crystal structure"

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Ocampo, Juan. "Etude des phénomènes d'interface dans la glace : adsorption, croissance des clathrates et désordre protonique : [thèse en partie soutenue sur un ensemble de travaux]." Grenoble 1, 1988. http://www.theses.fr/1988GRE10087.

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Etude depuis l'etat amorphe a 77 k jusqu'a l'etat hexagonal pres du point de fusion de l'evolution structurale et dynamique de la surface de la glace en contact ou non avec des gaz (he, kr, ar, n::(2), co::(2), nc::(4)h::(10)) ou des solides (sio::(2), pvc, h::(2)so::(4)). Approche thermodynamique (adsorption de gaz), cinetique (frittage et croissance de clathrates) et spectroscopique (rmn des protons). Mecanisme de reconstruction de la surface depuis l'adsorption jusqu'a la clathration, en tenant compte des coefficients de diffusion et des energies d'activation mesurees. Existence d'une couche quasi-liquide sur la surface de la glace pour des temperatures superieures a 238 k, et dans le cas des interfaces avec d'autres corps solides
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Mokhtari, Hossein. "Transmission electron microscopy of defects and internal fields in GaN structures." Thesis, University of Bristol, 2001. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.368206.

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Corkery, Robert, and robert corkery@anu edu au. "Artificial biomineralisation and metallic soaps." The Australian National University. Research School of Physical Sciences and Engineering, 1998. http://thesis.anu.edu.au./public/adt-ANU20080124.190014.

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In this thesis, geometry is used as a basis for conducting experiments aimed at growing and arranging inorganic minerals on curved interfaces. Mineralisation is directed using crystalline and liquid-crystalline metallic soaps and surfactant/water systems as templates.¶ A review of the history, syntheses, structure and liquid crystallinity of metallic soaps and other amphiphiles is presented as a foundation to understanding the interfacial architectures in mesostructured template systems in general.¶ In this study, a range of metallic soaps of varying chain length and cation type are synthesised and characterised to find potentially useful templates for mineral growth. These include alkaline-earth, transition metal, heavy metal and lanthanide soaps. These are systematically characterised using a variety of analytical techniques, including chemical analyses, x-ray diffraction (XRD) infrared spectroscopy (IR) and differential scanning calorimetry (DSC). Their molecular and crystal structures are studied using transmission electron microscopy (TEM), cryo-TEM, electron diffraction (ED), electron paramagnetic spin resonance (EPR), absorption spectroscopy (UV-VIS), high resolution laser spectroscopy, atomic force microscopy (AFM), nuclear magnetic resonance spectroscopy, scanning electron microscopy (SEM), electron dispersive x-ray analysis (EDXA), thermal gravimetric analysis (TGA) and magnetic measurements. Models for the molecular and crystal structures of metallic soaps are proposed. The soaps are predominantly lamellar crystalline or liquid crystalline lamellar rotor phases with tilted and/or untilted molecular constituents. These display evidence of varying degrees of headgroup organisation, including superstructuring and polymerisation. A single crystal structure is presented for a complex of pyridine with cobalt soap. Simple models for their structure are discussed in terms of their swelling properties in water and oils. Experiments are also presented to demonstrate the sorbent properties of aluminium soaps on oil spills.¶ The thermotropic liquid crystallinity of alkaline earth, transition metal, heavy metal and lanthanide soaps is investigated in detail. This is done to assess their suitability as templates, and to document their novel thermotropic behaviour, particularly the relatively unknown lanthanide soaps. Liquid crystalline behaviours are studied using high-temperature XRD (HTXRD), hot-stage optical microscopy and DSC. Models for a liquid crystalline phase progression from crystals to anisotropic liquids are discussed in terms of theories of self-assembly and interfacial curvature. The terminology required for this is drawn from various nomenclature systems for amphiphilic crystals and liquid crystals. General agreement with previous studies is reported for known soaps, while liquid crystallinity is demonstrated in the lanthanide and some non-lanthanide soaps for the first time. A general phase progression of crystalline lamellar through liquid crystalline lamellar to non-lamellar liquid crystalline is discussed in terms of models concerned with the molecular and crystal structures of the soaps and their phase transitions via headgroup and chain re-arrangements.¶ Experiments aimed at guiding growth of metal sulfides using metallic soaps as templates are described, and a model for this growth is discussed. Metal sulfides have been successfully grown by reacting crystalline and liquid crystalline transition metal and heavy metal soaps with H2S gas at room temperature and at elevated temperature. These have been characterised using XRD, TEM, ED and IR. Sulfide growth is demonstrated to be restricted and guided by the reacting soap template architecture. Zinc, cadmium, indium and lead soaps formed confined nanoparticles within the matrix of their reacting soap template. In contrast, curved and flat sheet-like structures, some resembling sponges were found in the products of sulfided iron, cobalt, nickel, copper, tin and bismuth soaps. A model to explain this behaviour is developed in terms of the crystal and liquid crystal structures of the soaps and the crystal structures of the metal sulfide particles.¶ Liquid crystalline iron soaps have been subjected to controlled thermal degradation yielding magnetic iron oxide nanoparticles. Some XRD and TEM evidence has been found for formation of magnetic mesostructures in heat-treated iron soaps. Models for the molecular and liquid crystalline structure of iron soaps, their thermotropic phase progression and eventual conversion to these magnetic products are discussed. Systematic syntheses of mesoporous silicates from sheeted clays are discussed.¶The templates that have been used are cationic surfactants and small, organic molecular salts. Experiments are reported where a cooperative self-assembly of surfactant/water/kanemite plus or minus salt and oils yields 'folded sheet materials' (FSM'S). Templating of kanemite has also been achieved using cobalt cage surfactants. A theoretical prediction of the specific surface areas and specific volumes of homologous sets of FSM's gave excellent agreement with measured values. The geometry and topology of the mesostructures are discussed. A theoretical model is also discussed regarding the curvature found in the sheets of natural clays , and results of templating clays and silica using metallic soaps are presented. Experiments and a model for low temperature nucleation and growth of microporous silicalite-1 are described in terms of silica templating by water clathrates.¶ Finally, the problem of finding minimal surface descriptions of crystal networks is addressed. Combinatoric methods are used to disprove the existence of possible embeddings of type I and II clathrate networks in non-self intersecting periodic minimal surfaces. The crystal network of the clathrate silicate, melanophlogite is successfully embedded in the WI-10 self-intersecting surface. Details of a previously unreported, genus-25 periodic surface with symmetry Im3m are discussed.
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Pignard, Stéphane. "Elaboration par MOCVD à injection, caractérisations structurale et physique de films d'oxydes magnétiques : hexaferrite BaFe12O19 et pérovskite à magnétorésistance géante La(1-x)MnO(3-delta)." Grenoble INPG, 1997. http://www.theses.fr/1997INPG0189.

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Un des problemes majeurs des procedes cvd reside dans le controle precis de la pression de vapeur des precurseurs, lorsque ceux-ci sont liquides ou solides. Un nouveau procede, brevete dans notre laboratoire, permet de resoudre ce probleme : il s'agit du procede cvd a injection. Son principe est base sur l'injection controlee de micro-quantites d'une solution contenant les precurseurs. Le premier objectif de ce travail a ete la construction et la mise au point d'une nouvelle enceinte d'elaboration de couches minces par voie cvd basee sur ce principe. Dans l'effort d'augmentation de la densite de stockage sur milieu magnetique, l'enregistrement perpendiculaire suscite depuis de nombreuses annees un interet de tout premier plan. L'hexaferrite de baryum bafe#1#2o#1#9 presente des caracteristiques interessantes pour cette application : les films doivent etre textures et convenablement dopes pour reduire le champ d'anisotropie. Jusqu'alors seules des techniques physiques de depot ont ete utilisees pour la synthese de telles couches. Nous avons etudie la possibilite d'elaborer des films de bafe#1#2o#1#9 par voie chimique au moyen du procede cvd a injection. Concernant la lecture des informations stockees, l'accroissement de la densite de stockage necessite l'utilisation de nouvelles tetes de lecture : dans ce domaine, les tetes magnetoresistives sont les plus prometteuses. Les recherches se sont recemment intensifiees avec la decouverte de la magnetoresistance colossale des composes la#1#-#xa#xmno#3#-# (a=sr,ca,ba). Nous nous sommes interesses aux manganites de lanthane lacunaires la#1#-#xmno#3#-#, deposes sous forme de couches minces par cvd a injection, dont les proprietes ont ete peu etudiees jusqu'a ce jour. Nous montrons que la technique de depot mise au point peut etre tres performante pour l'elaboration de tels films. Les proprietes structurales et physiques des couches la#1#-#xmno#3#-# sont etudiees : une magnetoresistance de 20%/tesla est obtenue a temperature ambiante
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Tallapally, Venkatesham. "Colloidal Synthesis and Photophysical Characterization of Group IV Alloy and Group IV-V Semiconductors: Ge1-xSnx and Sn-P Quantum Dots." VCU Scholars Compass, 2018. https://scholarscompass.vcu.edu/etd/5568.

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Nanomaterials, typically less than 100 nm size in any direction have gained noteworthy interest from scientific community owing to their significantly different and often improved physical properties compared to their bulk counterparts. Semiconductor nanoparticles (NPs) are of great interest to study their tunable optical properties, primarily as a function of size and shape. Accordingly, there has been a lot of attention paid to synthesize discrete semiconducting nanoparticles, of where Group III-V and II-VI materials have been studied extensively. In contrast, Group IV and Group IV-V based nanocrystals as earth abundant and less-non-toxic semiconductors have not been studied thoroughly. From the class of Group IV, Ge1-xSnx alloys are prime candidates for the fabrication of Si-compatible applications in the field of electronic and photonic devices, transistors, and charge storage devices. In addition, Ge1-xSnx alloys are potentials candidates for bio-sensing applications as alternative to toxic materials. Tin phosphides, a class of Group IV-V materials with their promising applications in thermoelectric, photocatalytic, and charge storage devices. However, both aforementioned semiconductors have not been studied thoroughly for their full potential in visible (Vis) to near infrared (NIR) optoelectronic applications. In this dissertation research, we have successfully developed unique synthetic strategies to produce Ge1-xSnx alloy quantum dots (QDs) and tin phosphide (Sn3P4, SnP, and Sn4P3) nanoparticles with tunable physical properties and crystal structures for potential applications in IR technologies. Low-cost, less-non-toxic, and abundantly-produced Ge1-xSnx alloys are an interesting class of narrow energy-gap semiconductors that received noteworthy interest in optical technologies. Admixing of α-Sn into Ge results in an indirect-to-direct bandgap crossover significantly improving light absorption and emission relative to indirect-gap Ge. However, the narrow energy-gaps reported for bulk Ge1-xSnx alloys have become a major impediment for their widespread application in optoelectronics. Herein, we report the first colloidal synthesis of Ge1-xSnx alloy quantum dots (QDs) with narrow size dispersity (3.3±0.5 – 5.9±0.8 nm), wide range of Sn compositions (0–20.6%), and composition-tunable energy-gaps and near infrared (IR) photoluminescence (PL). The structural analysis of alloy QDs indicates linear expansion of cubic Ge lattice with increasing Sn, suggesting the formation of strain-free nanoalloys. The successful incorporation of α-Sn into crystalline Ge has been confirmed by electron microscopy, which suggests the homogeneous solid solution behavior of QDs. The quantum confinement effects have resulted in energy gaps that are significantly blue-shifted from bulk Ge for Ge1-xSnx alloy QDs with composition-tunable absorption onsets (1.72–0.84 eV for x=1.5–20.6%) and PL peaks (1.62–1.31 eV for x=1.5–5.6%). Time-resolved PL (TRPL) spectroscopy revealed microsecond and nanosecond timescale decays at 15 K and 295 K, respectively owing to radiative recombination of dark and bright excitons as well as the interplay of surface traps and core electronic states. Realization of low-to-non-toxic and silicon-compatible Ge1-xSnx QDs with composition-tunable near IR PL allows the unprecedented expansion of direct-gap Group IV semiconductors to a wide range of biomedical and advanced technological studies. Tin phosphides are a class of materials that received noteworthy interest in photocatalysis, charge storage and thermoelectric devices. Dual stable oxidation states of tin (Sn2+ and Sn4+) enable tin phosphides to exhibit different stoichiometries and crystal phases. However, the synthesis of such nanostructures with control over morphology and crystal structure has proven a challenging task. Herein, we report the first colloidal synthesis of size, shape, and phase controlled, narrowly disperse rhombohedral Sn4P3, hexagonal SnP, and amorphous tin phosphide nanoparticles (NPs) displaying tunable morphologies and size dependent physical properties. The control over NP morphology and crystal phase was achieved by tuning the nucleation/growth temperature, molar ratio of Sn/P, and incorporation of additional coordinating solvents (alkylphosphines). The absorption spectra of smaller NPs exhibit size-dependent blue shifts in energy gaps (0.88–1.38 eV) compared to the theoretical value of bulk Sn3P4 (0.83 eV), consistent with quantum confinement effects. The amorphous NPs adopt rhombohedral Sn4P3 and hexagonal SnP crystal structures at 180 and 250 °C, respectively. Structural and surface analysis indicates consistent bond energies for phosphorus across different crystal phases, whereas the rhombohedral Sn4P3 NPs demonstrate Sn oxidation states distinctive from those of the hexagonal and amorphous NPs owing to complex chemical structure. All phases exhibit N(1s) and ʋ(N-H) energies suggestive of alkylamine surface functionalization and are devoid of tetragonal Sn impurities.
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Rong, Qiu Yi, and 邱奕榮. "The band structure in 2D hexagonal pipe photonic crystal." Thesis, 2006. http://ndltd.ncl.edu.tw/handle/58491984925513067779.

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碩士<br>國防大學中正理工學院<br>應用物理研究所<br>94<br>In this paper, the photonic crystal with two-dimensional hexagonal pipes structures is investigated. This photonic crystal includes the special case that with the two-dimensional hexagonal cylinders structure. In this investigation, we know that the energy band of the hexagonal cylinders structure photonic crystal will shift to lower frequency when the filling rate and dielectric coefficient increasing. And the width of complete gap will increase then decreasing. The structure of the Complete Gap is not effected by the alteration of dielectric coefficient. It would effect the width of band gap and frequencies when the dielectric coefficient been changed. In the different materials of hexagonal cylinders structure photonic crystal, the energy band gaps shift to lower frequencies when the dielectric coefficient increasing. When the cylinders radii are equal, the conditions of maximum gap been found. And in the hexagonal pipe structure photonic crystals, when the fitting materials are changed from cylinders to pipes, the energy band shift to higher frequencies just as the filling rate is decreasing. In this condition, it would be Complete Gape that it should not be Complete Gape. The Complete Gap of the hexagonal pipes structure photonic crystals would be found by this way.
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Liao, Tsu-Wei, та 廖梓為. "Single crystal growth and structure analysis of hexagonal tungsten bronzes in superconducting Rb0.23WO3+δ". Thesis, 2007. http://ndltd.ncl.edu.tw/handle/97246635678924299659.

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碩士<br>淡江大學<br>物理學系碩士班<br>95<br>Rubidium tungsten bronze RbxWOy (0.19< x< 0.33,2.9< y< 3.05) has been observed that the oxygen concentration dependent metal-nonmetal transition, and the rubidium and oxygen concentration dependent distribution for superconductivity critical temperature. In order to investigate the properties of RbxWOy more clearly, the preparation for single crystalline samples Rb0.23WOy (2.90≦y≦3.00) was carried out. The melting point of Rb0.23WOy increases as the oxygen concentration decreases. The melting point of Rb0.23WO3.00 is 1190oC and that of Rb0.23WO2.90 is 1210oC. And the size of single crystals affected by the cooling rate of calcination. The back-reflection Laue method presents p2mm symmetry along (1 0 0), and p6mm symmetry along (0 0 1) respectively for all single crystals with different oxygen concentration. The single crystalline Rb0.23WO3.00 was annealed in oxygen, and the superconductivity was observed above 3 K while the original material didn''t superconduct above 2 K, and the lattice parameter c decreased as the annealing times increased.
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Jain, Sanjeev. "Molecular structure of d(GTGTACAC) in the spermine-bound tetragonal and the spermine-free hexagonal crystal forms." 1990. http://catalog.hathitrust.org/api/volumes/oclc/22971322.html.

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Thesis (Ph. D.)--University of Wisconsin--Madison, 1990.<br>Typescript. Vita. eContent provider-neutral record in process. Description based on print version record. Includes bibliographical references.
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Yeh, Ching-Chung, and 葉精中. "Hexagonal, circular and new square structure photonic crystals-fabrication and optical property simulation." Thesis, 2008. http://ndltd.ncl.edu.tw/handle/70321046778096332949.

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碩士<br>國立中正大學<br>物理所<br>96<br>In this thesis, the electro-resist is firstly made with the pattern of hexagonal photonic crystal resonant cavity and circular photonic crystal on the SOI (silicon on insulator) using the E-beam lithography technique. The reactive ion etching (RIE) is then used to transfer the pattern of the electro-resist to the top layer of the SOI, and the SOI is soaked into the BOE (the mixed solvent of HF and NH4F) to remove the silica of the SOI to form the 3-D confinement. Once the sample is produced, the planer wave expansion (PWE) method and the finite difference time domain (FDTD) method are individually used to simulate the band structure, transmission spectra, resonance spectra, and Q factor in 2-D and 3-D structure. The result of simulation is further used to analyze the influence of the Q factor and resonance wavelength by varying the value of structure parameter. It is then expected to find the period or the filling ratio (radius/period) of the photonic crystal which corresponds to the communication wavelength. Finally, we compare the results of 2-D and 3-D simulation.
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Patil, S. S., E. Venugopal, S. Bhat, K. R. Mahadik, and Anant R. Paradkar. "Exploring Microstructural Changes in Structural Analogues of Ibuprofen-Hosted In Situ Gelling System and Its Influence on Pharmaceutical Performance." 2015. http://hdl.handle.net/10454/9394.

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No<br>The present work explores inner structuration of in situ gelling system consisting of glyceryl monooleate (GMO) and oleic acid (OA). The system under study involves investigation of microstructural changes which are believed to govern the pharmaceutical performance of final formulation. The changes which are often termed mesophasic transformation were analysed by small angle X-ray scattering (SAXS), differential scanning calorimetry (DSC), rheology and plane polarised light (PPL) microscopy. The current work revealed transformation of blank system from W/O emulsion to reverse hexagonal structure upon addition of structural analogues of ibuprofen. Such transformations are believed to occur due to increased hydrophobic volume within system as probed by SAXS analysis. The findings of SAXS studies were well supported by DSC, rheology and PPL microscopy. The study established inverse relationship between log P value of structural analogues of ibuprofen and the degree of binding of water molecules to surfactant chains. Such relationship had pronounced effect on sol-gel transformation process. The prepared in situ gelling system showed sustained drug release which followed Higuchi model.
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Book chapters on the topic "Hexagonal crystal structure"

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Suryanarayana, C., and M. Grant Norton. "Crystal Structure Determination. II: Hexagonal Structures." In X-Ray Diffraction. Springer US, 1998. http://dx.doi.org/10.1007/978-1-4899-0148-4_5.

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Li, Xiangyu, Baoji Ma, Bin Liu, Jinkui Cao, and Liangliang Li. "Microstructure of AZ31B Alloy Induced by Laser Shock." In Lecture Notes in Mechanical Engineering. Springer Nature Singapore, 2025. https://doi.org/10.1007/978-981-97-7887-4_63.

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Abstract Magnesium alloys have great potential in the field of biomedical degradable materials. However, their poor mechanical and corrosion resistance properties limit their applications. In this study, the AZ31B alloy with a compact hexagonal close-packed (HCP) crystal structure was selected as the material, as it tends to undergo twinning deformation rather than dislocation slip during plastic deformation due to its low stacking fault energy. The microstructures before and after LSP treatment were characterized using optical microscopy (OM), electron backscatter diffraction (EBSD), and X-ray diffraction (XRD). The results showed that the grain size was refined and exhibited a gradient distribution after LSP treatment. Electron backscatter diffraction (EBSD) was used to characterize the microstructure of LSP before and after treatment. The results showed that the grain size was refined after LSP treatment, and showed a gradient distribution trend.
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Meijer, Janne-Mieke. "Double Hexagonal Close Packed Structure Revealed in a Single Colloidal Crystal Grain by Bragg Rod Analysis." In Colloidal Crystals of Spheres and Cubes in Real and Reciprocal Space. Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-14809-0_3.

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Sursaeva, Vera G. "Effect of Hexagonal Crystal Structure Anisotropy on the Selective Grain Boundary Mobility during Texture Formation and Secondary Recrystallization in Zn." In Materials Science Forum. Trans Tech Publications Ltd., 2005. http://dx.doi.org/10.4028/0-87849-975-x.1231.

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Lindblom, G., L. B. Å. Johansson, G. Wikander, and P. O. Eriksson. "Spectroscopic Studies on Structure and Dynamics of Lyotropic Liquid Crystals: Cubic and Reversed Hexagonal Phases and Lipid Vesicles." In The Molecular Dynamics of Liquid Crystals. Springer Netherlands, 1994. http://dx.doi.org/10.1007/978-94-011-1168-3_23.

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Kurt, Huseyin, and J. M. D. Coey. "Magnetic and Electronic Properties of Thin Films of Mn-Ga and Mn-Ge Compounds with Cubic, Tetragonal and Hexagonal Crystal Structures." In Heusler Alloys. Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-21449-8_7.

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Müller, Ulrich, and Gemma de la Flor. "Derivation of crystal structures from closest packings of spheres." In Symmetry Relationships between Crystal Structures, 2nd ed. Oxford University PressOxford, 2024. https://doi.org/10.1093/oso/9780192858320.003.0014.

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Abstract A large number of crystal structures can be derived by partial occupation of interstices in closest packings of spheres. Examples are the rhombohedral, hexagonal and trigonal hettotypes that result from the partial occupation of octahedral voids in the hexagonal-closest packing of spheres. Other examplers are the hettotypes of the NaCl structure with a doubled unit cell and partial occupation of the octahedral voids, and the hetttotypes of the CaF2 type with a doubled unit cell and partial occupation of the tetrahedral voids.
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Desai, Neha, and Rajesh Kavade. "SYNTHESIS AND CHARACTERIZATION OF MoO3 NANORODS." In Futuristic Trends in Chemical Material Sciences & Nano Technology Volume 3 Book 25. Iterative International Publishers, Selfypage Developers Pvt Ltd, 2024. http://dx.doi.org/10.58532/v3becs25p1ch9.

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In this research, we synthesized MoO3 nanoparticles by chemical bath deposition. The synthesized MoO3 nanoparticles are well indexed to the hexagonal crystal structure. A morphological study reveals the presence of nanorods with a hexagonal crystal structure. An optical study shows a direct allowed band gap with absorption in the ultraviolet region. Compositional analysis shows the presence of molybdenum and oxygen in the synthesized nanoparticles.
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Glazer, A. M. "2. Symmetry." In Crystallography: A Very Short Introduction. Oxford University Press, 2016. http://dx.doi.org/10.1093/actrade/9780198717591.003.0002.

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In order to explain what crystals are and how their structures are described, we need to understand the role of symmetry, for this lies at the heart of crystallography. ‘Symmetry’ explains the different types of symmetry: rotational, mirror or reflection, point, chiral, and translation. There are thirty-two point groups and seven crystal systems, according to which symmetries are present. These are triclinic, monoclinic, orthorhombic, tetragonal, trigonal, hexagonal, and cubic. Miller indices, lattices, crystal structure, and space groups are described in more detail. Any normal crystal belongs to one of the 230 space group types. Crystallographers generally use the International Notation system to denote these space groups.
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Glazer, A. M. "3. Crystal structures." In Crystallography: A Very Short Introduction. Oxford University Press, 2016. http://dx.doi.org/10.1093/actrade/9780198717591.003.0003.

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‘Crystal structures’ describes the different types of close packing—hexagonal, cubic, face-centred cubic, and body-centred cubic—used to describe many simple inorganic structures, especially those of the elements. The reason for atoms to pack so closely together is to form the densest array possible to provide a stable structure. The ability of a chemical substance to adopt different crystal structures is called polymorphism, as displayed by carbon. Examples of simple inorganic structures, such as common salt, are explained along with organic crystal structures, and the different methods of crystal growth. Crystallography has also played a major part in determining the structures and activities of large biological molecules like DNA, RNA, proteins, and viruses.
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Conference papers on the topic "Hexagonal crystal structure"

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Dobrozhan, Andrii, Alina Khrypunova, Kseniia Minakova, Roman Zaitsev, Mykhailo Kirichenko, and Anton Drozdov. "Calculated Elastic Constants of CdS and CdTe Thin Films with Cubic and Hexagonal Crystal Structure for Stress Problems." In 2024 IEEE 5th KhPI Week on Advanced Technology (KhPIWeek). IEEE, 2024. https://doi.org/10.1109/khpiweek61434.2024.10878059.

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Islam, Md Maruf, Md Shakil Jahan Boni, Mehdi Hasan Chowdhury, and Kazi Tanvir Ahmmed. "Surface Plasmon Resonance Biosensor Based on Hexagonally Structured Photonic Crystal Fibre." In 2024 IEEE International Conference on Biomedical Engineering, Computer and Information Technology for Health (BECITHCON). IEEE, 2024. https://doi.org/10.1109/becithcon64160.2024.10962582.

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Maeda, Hiroshi, Hiroyuki Terashima, Yongmei Zhang, and Takuya Shinohara. "Hexagonal Resonator in Two Dimensional Photonic Crystal Structure." In 2011 Third International Conference on Intelligent Networking and Collaborative Systems (INCoS). IEEE, 2011. http://dx.doi.org/10.1109/incos.2011.99.

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Azizan, Muhammad Danial Haziq, Nurul Ashikin Binti Daud, Asrul Izam Bin Azmi, and Mohd Rashidi Bin Salim. "Characteristics of Hexagonal Photonic Crystal Width Modulated Cavity Waveguide Structure." In 2023 IEEE 21st Student Conference on Research and Development (SCOReD). IEEE, 2023. http://dx.doi.org/10.1109/scored60679.2023.10563625.

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Sechenykh, P. "MATHEMATICAL MODELING OF THE CRYSTAL STRUCTURE OF HEXAGONAL CLOSE-PACKED METALLS." In Mathematical modeling in materials science of electronic component. LCC MAKS Press, 2022. http://dx.doi.org/10.29003/m3083.mmmsec-2022/105-108.

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The paper presents the calculation of the metric parameters of crystalline compounds according to a given chemical formula and a space symmetry group. The hexagonal close-packed structure is considered
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Islam, Mohammad Rakibul, Aadreeta Hossain, Zareen Mustafa, and Tahia Tahsin. "A Novel Photonic Crystal Fiber Biosensor Using Single Hexagonal Lattice Structure." In 2020 11th International Conference on Electrical and Computer Engineering (ICECE). IEEE, 2020. http://dx.doi.org/10.1109/icece51571.2020.9393151.

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Hathcock, Megan, Bogdan Popa, and Kon-Well Wang. "Continuous Dirac Cone Evolution in Modulated Phononic Crystal." In ASME 2022 International Mechanical Engineering Congress and Exposition. American Society of Mechanical Engineers, 2022. http://dx.doi.org/10.1115/imece2022-95839.

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Abstract Dirac cones in the band structures of highly symmetric phononic crystal lattices have been extensively studied to produce unique acoustic phenomena. Traditionally, these interesting phenomena produced by Dirac cones occur at fixed frequencies, which cannot be adapted unless significant lattice material or geometric changes occur. To create tunable phononic structures, researchers have successfully utilized Miura-origami to modulate phononic inclusions between discrete high symmetry Bravais lattice configurations. However, the origami transformation between Bravais lattices is a continuous process, meaning that between the high symmetry Bravais lattices, the structure will transform into low symmetry lattices, which are largely unexplored. In this work, we study the perturbation of a hexagonal phononic lattice away from high symmetry. Interestingly, we see the Dirac cone at the K point of the Brillouin zone for the hexagonal lattice persist through the lattice modulation, despite loss of symmetry. Using this insight, we propose an origami phononic structure capable of continuous adjustment and refinement of Dirac cone frequency. Ultimately, we demonstrate continuous Dirac cone modulation for beam forming with the proposed origami phononic structure.
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Mohammadi, Saeed, Abdelkrim Khelif, Ryan Westafer, Eric Massey, William D. Hunt, and Ali Adibi. "Full Band-Gap Silicon Phononic Crystals for Surface Acoustic Waves." In ASME 2006 International Mechanical Engineering Congress and Exposition. ASMEDC, 2006. http://dx.doi.org/10.1115/imece2006-16227.

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Periodic elastic structures, called phononic crystals, show interesting frequency domain characteristics that can greatly influence the performance of acoustic and ultrasonic devices for several applications. Phononic crystals are acoustic counterparts of the extensively-investigated photonic crystals that are made by varying material properties periodically. Here we demonstrate the existence of phononic band-gaps for surface acoustic waves (SAWs) in a half-space of two dimensional phononic crystals consisting of hexagonal (honeycomb) arrangement of air cylinders in a crystalline Silicon background with low filling fraction. A theoretical calculation of band structure for bulk wave using finite element method is also achieved and shows that there is no complete phononic band gap in the case of the low filling fraction. Fabrication of the holes in Silicon is done by optical lithography and deep Silicon dry etching. In the experimental characterization, we have used slanted finger interdigitated transducers deposited on a thin layer of Zinc oxide (sputtered on top of the phononic crystal structure to excite elastic surface waves in Silicon) to cover a wide range of frequencies. We believe this to be the first reported demonstration of phononic band-gap for SAWs in a hexagonal lattice phononic crystal at such a high frequency.
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Waghmare, Madhavi H., and K. T. V. Reddy. "Analysisof Photonic bandgap structure in 2-D hexagonal and square lattice structure of photonic crystal." In 2014 International Conference on Advances in Communication and Computing Technologies (ICACACT). IEEE, 2014. http://dx.doi.org/10.1109/eic.2015.7230704.

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Vlasova, A. M. "Parallel computing for the simulation of deformation of hexagonal close-packed crystal (HCP)." In PROCEEDINGS OF THE INTERNATIONAL CONFERENCE ON PHYSICAL MESOMECHANICS. MATERIALS WITH MULTILEVEL HIERARCHICAL STRUCTURE AND INTELLIGENT MANUFACTURING TECHNOLOGY. AIP Publishing, 2020. http://dx.doi.org/10.1063/5.0034508.

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Reports on the topic "Hexagonal crystal structure"

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Kirchhoff, Helmut, and Ziv Reich. Protection of the photosynthetic apparatus during desiccation in resurrection plants. United States Department of Agriculture, 2014. http://dx.doi.org/10.32747/2014.7699861.bard.

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In this project, we studied the photosynthetic apparatus during dehydration and rehydration of the homoiochlorophyllous resurrection plant Craterostigmapumilum (retains most of the photosynthetic components during desiccation). Resurrection plants have the remarkable capability to withstand desiccation, being able to revive after prolonged severe water deficit in a few days upon rehydration. Homoiochlorophyllous resurrection plants are very efficient in protecting the photosynthetic machinery against damage by reactive oxygen production under drought. The main purpose of this BARD project was to unravel these largely unknown protection strategies for C. pumilum. In detail, the specific objectives were: (1) To determine the distribution and local organization of photosynthetic protein complexes and formation of inverted hexagonal phases within the thylakoid membranes at different dehydration/rehydration states. (2) To determine the 3D structure and characterize the geometry, topology, and mechanics of the thylakoid network at the different states. (3) Generation of molecular models for thylakoids at the different states and study the implications for diffusion within the thylakoid lumen. (4) Characterization of inter-system electron transport, quantum efficiencies, photosystem antenna sizes and distribution, NPQ, and photoinhibition at different hydration states. (5) Measuring the partition of photosynthetic reducing equivalents between the Calvin cycle, photorespiration, and the water-water cycle. At the beginning of the project, we decided to use C. pumilum instead of C. wilmsii because the former species was available from our collaborator Dr. Farrant. In addition to the original two dehydration states (40 relative water content=RWC and 5% RWC), we characterized a third state (15-20%) because some interesting changes occurs at this RWC. Furthermore, it was not possible to detect D1 protein levels by Western blot analysis because antibodies against other higher plants failed to detect D1 in C. pumilum. We developed growth conditions that allow reproducible generation of different dehydration and rehydration states for C. pumilum. Furthermore, advanced spectroscopy and microscopy for C. pumilum were established to obtain a detailed picture of structural and functional changes of the photosynthetic apparatus in different hydrated states. Main findings of our study are: 1. Anthocyan accumulation during desiccation alleviates the light pressure within the leaves (Fig. 1). 2. During desiccation, stomatal closure leads to drastic reductions in CO2 fixation and photorespiration. We could not identify alternative electron sinks as a solution to reduce ROS production. 3. On the supramolecular level, semicrystalline protein arrays were identified in thylakoid membranes in the desiccated state (see Fig. 3). On the electron transport level, a specific series of shut downs occur (summarized in Fig. 2). The main events include: Early shutdown of the ATPase activity, cessation of electron transport between cyt. bf complex and PSI (can reduce ROS formation at PSI); at higher dehydration levels uncoupling of LHCII from PSII and cessation of electron flow from PSII accompanied by crystal formation. The later could severe as a swift PSII reservoir during rehydration. The specific order of events in the course of dehydration and rehydration discovered in this project is indicative for regulated structural transitions specifically realized in resurrection plants. This detailed knowledge can serve as an interesting starting point for rationale genetic engineering of drought-tolerant crops.
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