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Relevant bibliographies by topics / Structural phase

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Academic literature on the topic 'Structural phase'

Author: Grafiati

Published: 5 June 2025

Last updated: 24 June 2025

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Journal articles on the topic "Structural phase"

1

Aftandiliants, Ye G. "Modelling of structure forming in structural steels." Naukovij žurnal «Tehnìka ta energetika» 11, no. 4 (2020): 13–22. http://dx.doi.org/10.31548/machenergy2020.04.013.

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The study showed that the influence of alloying elements on the secondary structure formation of the steels containing from 0.19 to 0.37 wt. % carbon; 0.82-1.82 silicon; 0.63-3.03 manganese; 1.01-3.09 chromium; 0.005-0.031 nitrogen; up to 0.25 wt.% vanadium and austenite grain size is determined by their change in the content of vanadium nitride phase in austenite, its alloying and overheating above tac3, and the dispersion of ferrite-pearlite, martensitic and bainitic structures is determined by austenite grain size and thermal kinetic parameters of phase transformations. Analytical dependencies are defined that describe the experimental data with a probability of 95% and an error of 10% to 18%. An analysis results of studying the structure formation of structural steel during tempering after quenching show that the dispersion and uniformity of the distribution of carbide and nitride phases in ferrite is controlled at complete austenite homogenization by diffusion mobility and the solubility limit of carbon and nitrogen in ferrite, and secondary phase quantity in case of the secondary phase presence in austenite more than 0.04 wt. %. Equations was obtained which, with a probability of 95% and an error of 0.7 to 2.6%, describe the real process.

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Knight, Kevin S., William G. Marshall, C. Michael B. Henderson, and Andrew A. Chamberlain. "Equation of state and a high-pressure structural phase transition in the gillespite-structured phase Ba0.5Sr0.5CuSi4O10." European Journal of Mineralogy 25, no. 6 (2014): 909–17. http://dx.doi.org/10.1127/0935-1221/2013/0025-2333.

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Aftandiliants, Ye G. "Modelling of phase transformations in structural steels." Naukovij žurnal «Tehnìka ta energetika» 11, no. 2 (2020): 15–20. http://dx.doi.org/10.31548/machenergy2020.02.015.

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A. Cowley, R., and S. M. Shapiro. "Structural Phase Transitions." Journal of the Physical Society of Japan 75, no. 11 (2006): 111001. http://dx.doi.org/10.1143/jpsj.75.111001.

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Kubicki, Maciej. "Structural Aspects of Phase Transitions." Solid State Phenomena 112 (May 2006): 1–20. http://dx.doi.org/10.4028/www.scientific.net/ssp.112.1.

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There are two kinds of structural transformations in the crystalline solid state: solid state reactions, in which the product chemically different from the starting material can be isolated, and polymorphic transitions, when the phases have different organization of identical molecules in the crystal structures. As a consequence, the starting and the final phases of a solid state reaction differ in the melt and vapor, while different polymorphic modifications are identical in melt or gas phase. Some examples of the different phase transitions in the solid state are described in detail: the π-molecular complexes, the hydrogen-bond transformations and the reversible single crystal - twin transition.

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Yurov, V. M., S. A. Guchenko, V. Ch Laurinas, and O. N. Zavatskaya. "Structural phase transition in surface layer of metals." Bulletin of the Karaganda University. "Physics" Series 93, no. 1 (2019): 50–60. http://dx.doi.org/10.31489/2019ph1/50-60.

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KAR, MANORANJAN, N. RAMA KRISHNAN, INDRAJIT TALUKDAR, and K. ACHARYYA. "STRUCTURAL TRANSITION OF NANOCRYSTALLINE TiO2." International Journal of Nanoscience 10, no. 01n02 (2011): 59–63. http://dx.doi.org/10.1142/s0219581x11007648.

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Nanocrystalline TiO 2 sample was prepared by high-energy ball mill method. A known quantity of anatase phase- TiO 2 was milled for 83 h in air. The samples were collected at intervals of 5 h of milling. The XRD patterns were recorded for all the samples. The crystal structure changed from anatase phase for bulk material to rutile-rich phase for nanocrystalline material. Nanocrystalline TiO 2, which is a mixture of anatase, rutile, and srilankite phase, was prepared by milling for 60 h. The XRD pattern of unmilled anatase phase of TiO 2 could be refined with I41/amd space group. The crystallite size of the TiO 2 was found to decrease with milling time upto 50 h and then the size of rutile phase increases while the sizes of anatase and srilankite phases remain constant upto 60 h of milling. After 60 h, the sizes of all the phases remain constant. The average crystallite size for rutile phase is found to be 12 nm after 60 h of milling.

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Hou, Zhi Yao, Xiao Di Wang, Jun Wang, and Bin Zhu. "Structural Studies on Ceria-Carbonate Composite Electrolytes." Key Engineering Materials 368-372 (February 2008): 278–81. http://dx.doi.org/10.4028/www.scientific.net/kem.368-372.278.

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This paper studied structures of ceria-carbonate two-phase composites, with an emphasis on the interfacial structures and interactions between the two constituent phases of ceria and carbonate. The phase structure was analyzed by DSC, XRD and SEM. The IR measurements were carried out to identify the bonding situations and interfaces. Some new absorptions and wavenumber shifts of the bands appeared in IR spectra. There are strong indications of the interfacial phenomena exist in the two-phase composites through comparison between the two-phase composite with each individual constituent phases. The results opened a new interesting subject on the two-phase composite structures with significant importance for applications in advanced low temperature (300-600°C) SOFC.

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Weakley, T. J. R., E. R. Ylvisaker, R. J. Yager, et al. "Phase transitions in K2Cr2O7 and structural redeterminations of phase II." Acta Crystallographica Section B Structural Science 60, no. 6 (2004): 705–15. http://dx.doi.org/10.1107/s010876810402333x.

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Crystals of phase II K2Cr2O7, potassium dichromate, space group P\overline 1, grown from aqueous solution undergo a first-order transition to phase I, space group reportedly P21/n, at a phase-transition temperature, T PT, of 544 (2) K on first heating; the corresponding transition on cooling is at 502 (2) K. The endotherm on subsequent heatings occurs reproducibly at T PT = 531 (2) K. Mass loss between ca 531 and 544 K, identified as included water, is rapid and continues more slowly to higher temperatures for a total loss of ca 0.20%. The higher T PT on first heating is associated with the increasing pressure of superheated water occupying inclusion defects. The latent diagonal glide plane in phase II allows the structure of phase I to be inferred. The triclinic structure at 296 K has been independently redetermined. Normal probability analysis shows high consistency between the resulting and previous atomic coordinates, but with uncertainties reduced by a factor of ca 2. The earlier uncertainties are systematically underestimated by a comparable factor. The structure of phase IIb, space group A2/a on transposing axes, was determined at ca 300 K by Krivovichev et al. [Acta Cryst. (2000), C56, 629–630]. The first-order transition between phases I and II arises from the ca 60° relative rotation of terminal O atoms in each tetrahedron as the n glide plane is gained or lost. A transition between phases IIb and I, also of first order, is likely but not between phases II and IIb. An intermediate phase may exist between phases IIb and I.

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Tkachuk, O., Ya Matychak, I. Pohrelyuk, and V. Fedirko. "Diffusion of Nitrogen and Phase—Structural Transformations in Titanium." METALLOFIZIKA I NOVEISHIE TEKHNOLOGII 36, no. 8 (2016): 1079–89. http://dx.doi.org/10.15407/mfint.36.08.1079.

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Dissertations / Theses on the topic "Structural phase"

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Giddy, Andrew Peter. "Computational studies of structural phase transitions." Thesis, University of Cambridge, 1991. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.239582.

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Gibson, Robert Gould. "Phase variability of structural transfer functions." Thesis, Massachusetts Institute of Technology, 1986. http://hdl.handle.net/1721.1/15023.

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Thesis (M.S.)--Massachusetts Institute of Technology, Dept. of Mechanical Engineering, 1986.<br>MICROFICHE COPY AVAILABLE IN ARCHIVES AND ENGINEERING<br>Bibliography: leaf 84.<br>by Robert Gould Gibson.<br>M.S.

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Jia, Zhihong. "Structural modulation and phase transitions in melilites." [S.l.] : [s.n.], 2005. http://archiv.ub.uni-marburg.de/diss/z2005/0066/.

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Jackson, Andrew N. "Structural phase behaviour via Monte Carlo techniques." Thesis, University of Edinburgh, 2001. http://hdl.handle.net/1842/4850.

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There are few reliable computational techniques applicable to the problem of structural phase behaviour. This is starkly emphasised by the fact that there are still a number of unanswered questions concerning the solid state of some of the simplest models of matter. To determine the phase behaviour of a given system we invoke the machinery of statistical physics, which identifies the equilibrium phase as that which minimises the free-energy. This type of problem can only be dealt with fully via numerical simulation, as any less direct approach will involve making some uncontrolled approximation. In particular, a numerical simulation can be used to evaluate the free-energy difference between two phases if the simulation is free to visit them both. However, it has proven very difficult to find an algorithm which is capable of efficiently exploring two different phases, particularly when one or both of them is a crystalline solid. This thesis builds on previous work (Physical Review Letters 79 p.3002), exploring a new Monte Carlo approach to this class of problem. This new simulation technique uses a global coordinate transformation to switch between two different crystalline structures. Generally, this `lattice switch' is found to be extremely unlikely to succeed in a normal Monte Carlo simulation. To overcome this, extended-sampling techniques are used to encourage the simulation to visit `gateway' microstates where the switch will be successful. After compensating for this bias in the sampling, the free-energy difference between the two structures can be evaluated directly from their relative probabilities. As concrete examples on which to base the research, the lattice-switch Monte Carlo method is used to determine the free-energy difference between the face-centred cubic (fcc) and hexagonal close-packed (hcp) phases of two generic model systems --- the hard-sphere and Lennard-Jones potentials. The structural phase behaviour of the hard-sphere solid is determined at densities near melting and in the close-packed limit. The factors controlling the efficiency of the lattice-switch approach are explored, as is the character of the `gateway' microstates. The face-centred cubic structure is identified as the thermodynamically stable phase, and the free-energy difference between the two structures is determined with high precision. These results are shown to be in complete agreement with the results of other authors in the field (published during the course of this work), some of whom adopted the lattice-switch method for their calculations. Also, the results are favourably compared against the experimentally observed structural phase behaviour of sterically-stabilised colloidal dispersions, which are believed to behave like systems of hard spheres. The logical extension of the hard sphere work is to generalise the lattice-switch technique to deal with `softer' systems, such as the Lennard-Jones solid. The results in the literature for the structural phase behaviour of this relatively simple system are found to be completely inconsistent. A number of different approaches to this problem are explored, leading to the conclusion that these inconsistencies arise from the way in which the potential is truncated. Using results for the ground-state energies and from the harmonic approximation, we develop a new truncation scheme which allows this system to be simulated accurately and efficiently. Lattice-switch Monte Carlo is then used to determine the fcc-hcp phase boundary of the Lennard-Jones solid in its entirety. These results are compared against the experimental results for the Lennard-Jones potential's closest physical analogue, the rare-gas solids. While some of the published rare-gas observations are in approximate agreement with the lattice-switch results, these findings contradict the widely held belief that fcc is the equilibrium structure of the heavier rare-gas solids for all pressures and temperatures. The possible reasons for this disagreement are discussed. Finally, we examine the pros and cons of the lattice-switch technique, and explore ways in which it can be extended to cover an even wider range of structures and interactions.

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McLinko, Ryan (Ryan M. ). "Conceptual Phase Structural Design Tool for Microsatellites." Thesis, Massachusetts Institute of Technology, 2011. http://hdl.handle.net/1721.1/67068.

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Thesis (S.M.)--Massachusetts Institute of Technology, Dept. of Aeronautics and Astronautics, 2011.<br>This electronic version was submitted by the student author. The certified thesis is available in the Institute Archives and Special Collections.<br>Cataloged from student submitted PDF version of thesis.<br>Includes bibliographical references (p. 122-124).<br>Gaining traction or momentum in the conceptual design phase for a complex system can be an arduous and daunting process, whether the complex system being designed is a satellite, airplane, car, or one of countless other systems. The design of small satellites is particularly affected by the difficulties in gaining traction since most of the customized tools that exist are proprietary, a significant experience base is required to be able to perform system level design trades, and the issue that most satellites serve one-of-a-kind applications. Of the subsystems in a satellite, the structures subsystem (along with other "downstream" subsystems, such as power and thermal), tends to be less mature during the conceptual design phase since its design depends strongly on the particular designs and requirements of each of the other subsystems, which also take time to mature. The Conceptual Phase Structural Design Tool for Microsatellites (SDT) facilitates the development of potential small satellite structural architectures and the selection of an initial satellite architecture to use in the detailed design process. The tool is capable of evaluating the strength, stiffness, mass, and inertial properties of a satellite architecture and is customizable to a wide range of potential missions by allowing for a number of structural architectures and customizable component placement. Furthermore, the tool has been developed with two key niches in mind. First, it is available to students with little to no satellite design experience, thus enabling a greater number of people, including those who are unfamiliar with the process of structural design at the beginning of the program, to design higher quality spacecraft from the start. Second, it is open source and deployable in a state that is usable and customizable by members of the satellite design industry.<br>by Ryan McLinko.<br>S.M.

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Wilding, Nigel Blair. "Studies of structural patterns at phase transitions." Thesis, University of Edinburgh, 1991. http://hdl.handle.net/1842/13233.

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The work described in this thesis comprises two distinct components. In the first part, Monte-Carlo computer simulation methods are employed within a finite-size scaling framework to investigate both universal and non-universal behaviour in two scalar models, the 1-d φ<SUP>4</SUP> model and the 2-d Lennard-Jones fluid. In both these models the properties of interest are obtained from studies of the large-length scale configurational patterns via measurements of the probability distribution function (PDF) of the coarse-grained (block) ordering variable. For the 1-d φ<SUP>4</SUP> model, simulations are employed to obtain the block PDF of the spin variable. This function is shown to map onto an analytically-derived expression for the 1-d Ising chain, thus exposing the model's essentially Ising-like character. It is further demonstrated that the corrections to the limiting form of the block PDF reflect system-specific features of the 1-d φ<SUP>4</SUP> model associated with its elementary excitations. In the 2-d Lennard-Jones fluid, the combined use of simulation and finite-size scaling is shown to provide a powerful method for accurately determining the location of the liquid-vapour coexistence curve and critical point. At the critical point, the limiting form of the coarse-grained density distribution is found to collapse onto a previously determined function characteristic of the 2-d Ising model, thereby confirming and clarifying fluid-magnet universality. Clear evidence is also presented for mixing of the temperature and chemical potential in the two relevant scaling fields-a phenomenon responsible for the failure of the law of rectilinear diameter. As an addendum, a discussion is given of the prospects for generalising to fluids, the cluster updating techniques recently developed to reduce critical slowing down in simulations of spin systems.

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Allen, Patryck Kevyn Kidd. "Structural studies of lead-free piezoelectrics with the fresnoite structure type." Thesis, The University of Sydney, 2012. http://hdl.handle.net/2123/11986.

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The lead free piezoelectric fresnoite A2M3O8 (A = Ba, Sr, K, Cs; M = Ti, V, Si, Ge) modulated structure type has been investigated owing to its potential to exhibit excellent piezoelectric response coefficients. Ba2TiSi2O8, Sr2TiSi2O8, and Ba2TiGe2O8 end members in addition to members of the Ba2xSr2-2xTiSi2O8, Ba2xSr2 2xTiGe2O8, Ba2TiGe2ySi2 2yO8, and BaSrTiGe2ySi2 2yO8 series were synthesised and characterised using a combination of variable temperature diffraction techniques. The Ba2TiSi2O8 and Sr2TiSi2O8 modulated structures at ambient temperature were characterised using neutron powder diffraction for the first time. Variable temperature synchrotron X ray diffraction data showed a new means of identifying the incommensurate to prototypic structural phase transition at 433 K. Resonant ultrasound spectroscopy has shown coupling between the elastic moduli and structural changes in fresnoite samples. Polycrystalline Sr2TiSi2O8 samples were shown to undergo a first order phase transition from a two phase mixture of incommensurately modulated tetragonal and orthorhombic phases to a single incommensurately modulated orthorhombic phase that is complete by 567 K. The proportion of the orthorhombic phase Sr2TiSi2O8 samples was shown to slowly decrease on cooling to 125 K. The Sr2TiSi2O8 structure was also shown to undergo an additional phase transition from the incommensurately modulated orthorhombic phase to a tetragonal phase at 1323 K for the first time. The inclusion of barium or germanium into the Sr2TiSi2O8 structure was shown to suppress the formation of the orthorhombic phase at ambient temperature and elevated temperatures. New phase diagrams for the Ba2xSr2-2xTiSi2O8 and Sr2TiGe2ySi2 2yO8 systems summarise the phase transitions investigated. The intrinsic piezoelectric coefficients were calculated to be approximately 5 pm V 1 and 27 pm V 1 for polycrystalline samples of Ba2TiSi2O8 and Sr2TiSi2O8 respectively and compared to common piezoelectric materials.

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Rabe, Karin M. (Karin Maria). "Ab initio statistical mechanics of structural phase transitions." Thesis, Massachusetts Institute of Technology, 1987. http://hdl.handle.net/1721.1/14630.

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Warren, Michele Carol. "Ab initio lattice dynamics and structural phase transitions." Thesis, University of Edinburgh, 1997. http://hdl.handle.net/1842/14635.

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Prediction of the conditions required for the transformation of one phase of a mineral into another has long been a goal of condensed matter physics. This is especially desirable for phase transitions which are believed to be involved in geological processes, but for which the conditions of temperature or pressure are hard to reproduce experimentally. This thesis examines a number of structural phase transitions including those of MgSiO<SUB>3</SUB> perovskite, which is thought to form the largest part of the Earth's mantle and of ZrO<SUB>2</SUB> which plays an important role in inhibiting crack formation in ceramics. These phase transitions, in which an alternative phase may be reached by continuous distortions of the structure on an atomic level, are examined primarily through the use of first principles electronic structure calculations. Existing first principles techniques were extended to facilitate determination of the equilibrium structure by relaxation of the unit cell and the calculation of the lattice dynamics of complex phases. The distortion involved in most of the phase transitions studied is found to reflect the normal vibrational modes of one or both phases. The phase transitions of MgSiO<SUB>3</SUB> are found to be well described by only a few normal modes of the highest-symmetry cubic phase, dominated by two modes involving tilting of the SiO<SUB>6</SUB> octahedra. These modes resemble rigid unit modes, in which SiO<SUB>6</SUB> octahedra are assumed to remain perfectly rigid but may rotate with respect to other octahedra, whilst preserving linkages between them. The extent to which such simple modes are an accurate description of the dynamics of MgSiO<SUB>3</SUB>, BaZrO<SUB>3</SUB> and SiO<SUB>2</SUB> is investigated by way of structural analysis and lattice dynamics of both stable and metastable phases. Both simple models deduced from the lattice dynamical analysis and molecular dynamics using forces calculated from first principles are used to estimate transition temperatures for thermally induced phase transitions in MgSiO<SUB>3</SUB>.

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Zierenberg, Johannes. "From Particle Condensation to Polymer Aggregation: Phase Transitions and Structural Phases in Mesoscopic Systems." Doctoral thesis, Universitätsbibliothek Leipzig, 2016. http://nbn-resolving.de/urn:nbn:de:bsz:15-qucosa-197255.

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Die vorliegende Arbeit befasst sich mit den Gleichgewichtseigenschaften und Phasenübergängen in verdünnten Teilchen- und Polymersystemen, mit einem Fokus auf Teilchenkondensation und Polymeraggregation. Dazu werden sowohl analytische Argumente als auch hochentwickelte Monte Carlo Simulationen verwendet. Um die in dieser Arbeit erreichten Systemgrößen zu simulieren, wurde eine parallele Version der multikanonischen Methode entwickelt. Die Leistungsfähigkeit dieser Erweiterung wird an mehreren relevanten Beispielen demonstriert. Um Teilchenkondensation und Polymeraggregation in finiten Systemen und in geometrisch beschränkten Strukturen besser zu verstehen, wird der Einfluss von verschiedenen Parametern auf die jeweiligen Übergange untersucht. Dies beinhaltet unter anderem die Systemgröße und Dichte, sowie im Speziellen für semiflexible Polymere deren Steifigkeit. Betrachtet werden sowohl kanonische Observablen (Energie, Tropfen- bzw. Aggregatgröße, etc.) mit der dazugehörigen Übergangstemperatur und -breite, als auch eine mikrokanonische Analyse sowie die Barrieren der Freien Energie. Für semiflexible Polymere wird insbesondere der Einfluss von Steifigkeit auf die resultierende Struktur der Aggregate untersucht, die von amorphen Kugeln für flexible Polymere bis hin zu verdrehten Bündeln für steifere Polymere reichen. Ein weiterer Fokus liegt auf der Untersuchung von Übereinstimmungen zwischen den generischen Mechanismen in Kondensation und Aggregation: dem Übergang zwischen einer homogenen Phase und einer inhomogenen (gemischten) Phase. Auf diesem Niveau kann man Polymeraggregation als Kondensation von ausgedehnten Objekten verstehen. Dies zeigt sich vor allem in dem Skalierungsverhalten von kanonischen und mikrokanonischen Observablen, insbesondere an einem unerwarteten aber konsistenten Bereich für mittelgroße (mesoskopische) Systemgrößen.

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Books on the topic "Structural phase"

1

Müller, K. Alex, and Harry Thomas, eds. Structural Phase Transitions II. Springer Berlin Heidelberg, 1991. http://dx.doi.org/10.1007/978-3-662-10113-1.

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Müller, K. Alex. Structural Phase Transitions II. Springer Berlin Heidelberg, 1991.

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1945-, Sigov A. S., ed. Defects and structural phase transitions. Gordon and Breach Science Publishers, 1988.

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Morán-López, J. L., F. Mejía-Lira, and J. M. Sanchez, eds. Structural and Phase Stability of Alloys. Springer US, 1992. http://dx.doi.org/10.1007/978-1-4615-3382-5.

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Fujimoto, Minoru. The Physics of Structural Phase Transitions. Springer New York, 1997. http://dx.doi.org/10.1007/978-1-4757-2725-8.

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1950-, Morán-López J. L., Mejía-Lira F, and Sanchez J. M, eds. Structural and phase stability of alloys. Plenum Press, 1992.

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Ghose, S., J. M. D. Coey, and E. Salje, eds. Structural and Magnetic Phase Transitions in Minerals. Springer New York, 1988. http://dx.doi.org/10.1007/978-1-4612-3862-1.

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Ghose, S. Structural and Magnetic Phase Transitions in Minerals. Springer New York, 1988.

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1932-, Ghose S., Coey J. M. D, and Salje Ekhard K. H, eds. Structural and magnetic phase transitions in minerals. Springer-Verlag, 1988.

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Majumder, Arun. Structural evolution of Indian economy: Early phase. Manohar Publications, 1992.

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Book chapters on the topic "Structural phase"

1

Batsanov, Stepan S., and Andrei S. Batsanov. "Phase Transition." In Introduction to Structural Chemistry. Springer Netherlands, 2012. http://dx.doi.org/10.1007/978-94-007-4771-5_9.

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Fujita, F. E. "Structural Phase Transformation." In Physics of New Materials. Springer Berlin Heidelberg, 1998. http://dx.doi.org/10.1007/978-3-642-46862-9_6.

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Fujita, F. E. "Structural Phase Transformation." In Physics of New Materials. Springer Berlin Heidelberg, 1994. http://dx.doi.org/10.1007/978-3-662-00461-6_6.

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Tolédano, J. C., V. Janovec, V. Kopský, J. F. Scott, and P. Boček. "Structural phase transitions." In International Tables for Crystallography. International Union of Crystallography, 2006. http://dx.doi.org/10.1107/97809553602060000642.

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Tolédano, J. C., V. Janovec, V. Kopský, J. F. Scott, and P. Boček. "Structural phase transitions." In International Tables for Crystallography. International Union of Crystallography, 2013. http://dx.doi.org/10.1107/97809553602060000915.

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Puebla, Ricardo. "Structural Phase Transitions." In Equilibrium and Nonequilibrium Aspects of Phase Transitions in Quantum Physics. Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-030-00653-2_2.

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Mahtaney, Piya. "The Next Phase of Structural Transformation." In Structural Transformation. Springer Singapore, 2021. http://dx.doi.org/10.1007/978-981-33-4662-8_1.

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Strauch, D. "CaO: phase transition pressure, phase stability, phase diagram, ferroelectric phases transition." In New Data and Updates for several IIa-VI Compounds (Structural Properties, Thermal and Thermodynamic Properties, and Lattice Properties). Springer Berlin Heidelberg, 2014. http://dx.doi.org/10.1007/978-3-642-41461-9_74.

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Freeman, A. J. "Structural Stability of Intermetallic Compounds: A Computational Metallurgical Approach." In Alloy Phase Stability. Springer Netherlands, 1989. http://dx.doi.org/10.1007/978-94-009-0915-1_26.

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Newman, Kathie E., Jun Shen, Dan Teng, Bing-Lin Gu, Shang-Yuan Ren, and John D. Dow. "Electronic and Structural Properties of Ordered III–V Alloys." In Alloy Phase Stability. Springer Netherlands, 1989. http://dx.doi.org/10.1007/978-94-009-0915-1_40.

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Conference papers on the topic "Structural phase"

1

Emrose, Md Tanvir, and Georgios Veronis. "Multilayer structures based on phase-change materials for reconfigurable structural color generation." In Active Photonic Platforms (APP) 2024, edited by Ganapathi S. Subramania and Stavroula Foteinopoulou. SPIE, 2024. http://dx.doi.org/10.1117/12.3028387.

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Fromme, Paul, and Philip Loveday. "Guided ultrasonic wave phase and group velocity measurement." In Health Monitoring of Structural and Biological Systems XIX, edited by Zhongqing Su. SPIE, 2025. https://doi.org/10.1117/12.3052278.

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Pourmand, M., and Pankaj K. Choudhury. "Designing Reconfigurable Metamaterials Toward Structural Color Generation." In JSAP-Optica Joint Symposia. Optica Publishing Group, 2024. https://doi.org/10.1364/jsapo.2024.16p_b4_5.

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Dynamic color-generation structures provide higher resolution and scalability compared to the traditional pigmentation-based displays [1]. The main roadblock to the wide adoption of structural colors is the fixed optical response after the realization process. To address this issue, several kinds of tunability mechanisms have been introduced including the implementation of plasmonic nano-antennas enabled by liquid crystals [2] and plasmonic resonators exploiting stretchable materials [3]. The chalcogenide phase-change mediums- (PCMs) based plasmonic structures [7]. Herein, we propose an optimized PCM-integrated structure to generate a wide spectrum of colors.

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Smayev, M. P., P. A. Smirnov, I. A. Budagovsky, et al. "Laser Beam Structure Influence on Optical and Structural Modification of Phase-Change Materials." In 2024 International Conference Laser Optics (ICLO). IEEE, 2024. http://dx.doi.org/10.1109/iclo59702.2024.10623996.

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Daasch, Andreas, Matthias Schultalbers, and Ferdinand Svaricek. "Structural non-minimum phase systems." In 2016 American Control Conference (ACC). IEEE, 2016. http://dx.doi.org/10.1109/acc.2016.7525498.

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RAHMAN, ZAHIDUL, JOHN SPANOS, and CHENGCHIN CHU. "OPTICAL PATHLENGTH CONTROL EXPERIMENT ON JPL PHASE B TESTBED." In 34th Structures, Structural Dynamics and Materials Conference. American Institute of Aeronautics and Astronautics, 1993. http://dx.doi.org/10.2514/6.1993-1695.

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Lee, Moosung, Eeksung Lee, JaeHwang Jung, et al. "Quantifying structural alterations in Alzheimer's disease brains using quantitative phase imaging (Conference Presentation)." In Quantitative Phase Imaging III, edited by Gabriel Popescu and YongKeun Park. SPIE, 2017. http://dx.doi.org/10.1117/12.2251560.

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KINCAID, REX, and CHRISTINA BLOEBAUM. "THE DAMPER PLACEMENT PROBLEM FOR THE CSI-PHASE 1 EVOLUTIONARY MODEL." In 34th Structures, Structural Dynamics and Materials Conference. American Institute of Aeronautics and Astronautics, 1993. http://dx.doi.org/10.2514/6.1993-1655.

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Sobierajski, Ryszard, Jerzy Antonowicz, Klaus Sokolowski-Tinten, et al. "Ultrafast structural transformations in metals studied by time resolved XRD." In Advances in Ultrafast Condensed Phase Physics IV, edited by Stefan Haacke. SPIE, 2024. http://dx.doi.org/10.1117/12.3016739.

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Higuchi, Ken. "A piezoelectric linear motor driven by superposing standing waves with phase difference." In 36th Structures, Structural Dynamics and Materials Conference. American Institute of Aeronautics and Astronautics, 1995. http://dx.doi.org/10.2514/6.1995-1110.

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Reports on the topic "Structural phase"

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Ebeling, Robert, та Barry White. Load and resistance factors for earth retaining, reinforced concrete hydraulic structures based on a reliability index (β) derived from the Probability of Unsatisfactory Performance (PUP) : phase 2 study. Engineer Research and Development Center (U.S.), 2021. http://dx.doi.org/10.21079/11681/39881.

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This technical report documents the second of a two-phase research and development (R&D) study in support of the development of a combined Load and Resistance Factor Design (LRFD) methodology that accommodates geotechnical as well as structural design limit states for design of the U.S. Army Corps of Engineers (USACE) reinforced concrete, hydraulic navigation structures. To this end, this R&D effort extends reliability procedures that have been developed for other non-USACE structural systems to encompass USACE hydraulic structures. Many of these reinforced concrete, hydraulic structures are founded on and/or retain earth or are buttressed by an earthen feature. Consequently, the design of many of these hydraulic structures involves significant soil structure interaction. Development of the required reliability and corresponding LRFD procedures has been lagging in the geotechnical topic area as compared to those for structural limit state considerations and have therefore been the focus of this second-phase R&D effort. Design of an example T-Wall hydraulic structure involves consideration of five geotechnical and structural limit states. New numerical procedures have been developed for precise multiple limit state reliability calculations and for complete LRFD analysis of this example T-Wall reinforced concrete, hydraulic structure.

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Dayal, Kaushik. Dynamics of Structural Phase Transformations Using Molecular Dynamics. Defense Technical Information Center, 2013. http://dx.doi.org/10.21236/ada606824.

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Bernstein, N., M. D. Johannes, and Khang Hoang. Origin Of The Structural Phase Transition In Li7La3Zr2O12. Defense Technical Information Center, 2012. http://dx.doi.org/10.21236/ada567120.

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Bubacz, Jacob A., Hana T. Chmielewski, Alexander E. Pape, et al. Phase Space Dissimilarity Measures for Structural Health Monitoring. Office of Scientific and Technical Information (OSTI), 2011. http://dx.doi.org/10.2172/1029952.

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Axe, J. D., H. You, D. Hohlwein, et al. Structural phase transformations and high-T/sub c/ superconductivity. Office of Scientific and Technical Information (OSTI), 1987. http://dx.doi.org/10.2172/6312717.

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Nicolaides, Roy A. Computational Methods for Electromagnetic Scattering and Structural Phase Transitions. Defense Technical Information Center, 1997. http://dx.doi.org/10.21236/ada334839.

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Jorgensen, J. D., D. G. Hinks, D. M. Hatch, and R. M. Putnam. Structural phase transitions in BaMo/sub 6/S/sub 8/: Evidence for an incommensurate phase. Office of Scientific and Technical Information (OSTI), 1986. http://dx.doi.org/10.2172/6363215.

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Toulouse, J. Effect of point defects and disorder on structural phase transitions. Office of Scientific and Technical Information (OSTI), 1997. http://dx.doi.org/10.2172/481919.

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Partner, Heather L., Ramil Nigmatullin, Tobias Burgermeister, et al. Structural phase transitions and topological defects in ion Coulomb crystals. Office of Scientific and Technical Information (OSTI), 2014. http://dx.doi.org/10.2172/1164430.

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Migilori, A., Z. Fisk, Ming Lei, et al. Structural phase transitions on non-stoichiometric oxides and other materials. Office of Scientific and Technical Information (OSTI), 1996. http://dx.doi.org/10.2172/212687.

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