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Artykuły w czasopismach na temat „Liquid phase growth”

Autor: Grafiati

Data publikacji: 3 czerwca 2025

Data aktualizacji: 31 lipca 2025

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1

Pu, Yong Ping, Gong An Yang, Yun He Liang, Wen Hu Yang, and Jin Fei Wang. "Influence of Liquid Phase on Grain Growth of Ba_0.998La_0.002TiO₃ Ceramics." Key Engineering Materials 368-372 (February 2008): 461–64. http://dx.doi.org/10.4028/www.scientific.net/kem.368-372.461.

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The influence of liquid phase on grain growth of Ba0.998La0.002TiO3+xmol%TiO2 (x=0~5.0) ceramics sintered at 1350°C was investigated. The result showed that the liquid phase must present during grain growth; on the other hand, BaTiO3 grains must be dissolved, and then, precipitated from the liquid phase during the process of dissolution-precipitation. Otherwise, the grain growth was inhibited. The liquid phases of Ba6Ti17O4 and Ba2TiSi2O8 promoted grain growth due to high solution of BaTiO3 grains in the liquid phases. Ba2Ti2SiP2O13 liquid phase inhibited grain growth since BaTiO3 grains canno

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2

Oswald, Patrick, John Bechhoefer, and Francisco Melo. "Pattern Formation During the Growth of Liquid Crystal Phases." MRS Bulletin 16, no. 1 (1991): 38–45. http://dx.doi.org/10.1557/s0883769400057894.

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Liquid crystals, discovered just a century ago, have wide application to electrooptic displays and thermography. Their physical properties have also made them fascinating materials for more fundamental research.The name “liquid crystals” is actually a misnomer for what are more properly termed “mesophases,” that is, phases having symmetries intermediate between ordinary solids and liquids. There are three major classes of liquid crystals: nematics, smectics, and columnar mesophases. In nematics, although there is no correlation between positions of the rodlike molecules, the molecules tend to

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3

Mosses, Joanna, David A. Turton, Leo Lue, Jan Sefcik, and Klaas Wynne. "Crystal templating through liquid–liquid phase separation." Chemical Communications 51, no. 6 (2015): 1139–42. http://dx.doi.org/10.1039/c4cc07880b.

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4

Tian, Pin, Libin Tang, Jinzhong Xiang, et al. "Liquid-phase catalytic growth of graphene." Journal of Materials Chemistry C 10, no. 2 (2022): 571–78. http://dx.doi.org/10.1039/d1tc04187h.

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5

Syväjärvi, M., R. Yakimova, H. H. Radamson, et al. "Liquid phase epitaxial growth of SiC." Journal of Crystal Growth 197, no. 1-2 (1999): 147–54. http://dx.doi.org/10.1016/s0022-0248(98)00878-1.

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6

Chang, L. W., J. Gong, C. Y. Sun, and H. L. Hwang. "Liquid phase epitaxial growth of CuInS2." Thin Solid Films 144, no. 2 (1986): 229–39. http://dx.doi.org/10.1016/0040-6090(86)90416-5.

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7

Crisman, E. E., J. T. Daly, H. J. Gerritsen, and S. K. F. Karlsson. "Rapid liquid phase epitaxial growth studies." Solar Cells 21, no. 1-4 (1987): 458. http://dx.doi.org/10.1016/0379-6787(87)90163-3.

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8

Huang, Yuan Ming, Qing Lan Ma, and Bao Gai Zhai. "Effects of Cyclic Heating and Cooling on the Banana-Phase Growing Behaviors of Banana-Shaped Liquid Crystal 1,3-Phenylene-bis[4-(4-octyl phenylimino)methyl]benzoate." Key Engineering Materials 428-429 (January 2010): 322–25. http://dx.doi.org/10.4028/www.scientific.net/kem.428-429.322.

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The effects of cyclic heating and cooling on the banana-phase growth behaviors of the prototype banana-shaped liquid crystal 1,3-phenylene-bis[4-(4-octylphenylimino)methyl]benzoate were investigated with differential scanning calorimetry and polarized optical microscopy, respectively. Cyclic heating and cooling can reduce the phase transition temperatures and increase the domain sizes of the banana phases of the banana-shaped liquid crystal. These results can be interpreted in terms of the nucleation and growth of the banana phases out of its isotropic phase of the banana-shaped liquid crystal

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9

Peev, N. S. "Processes in phase boundary region during liquid phase growth." Crystal Research and Technology 48, no. 2 (2013): 116–26. http://dx.doi.org/10.1002/crat.201200323.

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10

Castro, Mário Rui da Costa Basílio e., Carla Ragonezi, Paulo Guilherme Leandro de Oliveira, and Maria Amely Zavattieri. "A Novelty System for Biotization of Plant Microshoots and Collection of Natural Compounds." Methods and Protocols 2, no. 1 (2019): 5. http://dx.doi.org/10.3390/mps2010005.

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An in vitro plant microshoot culture system composed of two phases; a liquid phase overlaid by a floating solid phase, which is described in detail herein. This system is designed to enable the extraction of natural compounds released/disseminated into the liquid phase during root growth, thus facilitating their processing and biochemical characterization. The solid phase holds the plant afloat and enables the simultaneous culture of a microorganism, yet avoiding its penetration into the liquid phase, where the roots are submerged. Both phases can be independently formulated as required for gr

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11

Altosaar, Mare, and Enn Mellikov. "CuInSe2Monograin Growth in CuSe-Se Liquid Phase." Japanese Journal of Applied Physics 39, S1 (2000): 65. http://dx.doi.org/10.7567/jjaps.39s1.65.

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12

Syväjärvi, M., R. Yakimova, L. G. Ivanov, and E. Janzén. "Growth of 4H-SiC from liquid phase." Materials Science and Engineering: B 46, no. 1-3 (1997): 329–32. http://dx.doi.org/10.1016/s0921-5107(96)02001-6.

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13

Peev, N. S. "Some correlations in liquid phase growth (I)." Crystal Research and Technology 25, no. 6 (1990): 653–59. http://dx.doi.org/10.1002/crat.2170250607.

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14

Peev, N. S. "Some correlations in liquid phase growth (II)." Crystal Research and Technology 25, no. 11 (1990): 1265–69. http://dx.doi.org/10.1002/crat.2170251107.

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15

Sadigh, Babak, Luis Zepeda-Ruiz, and Jonathan L. Belof. "Metastable–solid phase diagrams derived from polymorphic solidification kinetics." Proceedings of the National Academy of Sciences 118, no. 9 (2021): e2017809118. http://dx.doi.org/10.1073/pnas.2017809118.

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Nonequilibrium processes during solidification can lead to kinetic stabilization of metastable crystal phases. A general framework for predicting the solidification conditions that lead to metastable-phase growth is developed and applied to a model face-centered cubic (fcc) metal that undergoes phase transitions to the body-centered cubic (bcc) as well as the hexagonal close-packed phases at high temperatures and pressures. Large-scale molecular dynamics simulations of ultrarapid freezing show that bcc nucleates and grows well outside of the region of its thermodynamic stability. An extensive

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16

Feng Qiu, Feng Qiu, Yingfei Lv Yingfei Lv, Jianhua Guo Jianhua Guo, et al. "Growth and Raman spectra of GaSb quantum dots in GaAs matrices by liquid phase epitaxy." Chinese Optics Letters 10, s2 (2012): S21603–321606. http://dx.doi.org/10.3788/col201210.s21603.

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17

Enomoto, Hiroyuki, Hirokazu Yamanaka, Nion Sock Chang, Jae Soo Shin, and Hajime Ozaki. "Formation of Bi2212 Phase via Bi2201 Phase in Liquid-Phase Epitaxial Growth." Japanese Journal of Applied Physics 38, Part 2, No. 5A (1999): L501—L504. http://dx.doi.org/10.1143/jjap.38.l501.

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18

Hodas, N., A. Zuend, W. Mui, R. C. Flagan, and J. H. Seinfeld. "Influence of particle phase state on the hygroscopic behavior of mixed organic–inorganic aerosols." Atmospheric Chemistry and Physics Discussions 14, no. 23 (2014): 32935–77. http://dx.doi.org/10.5194/acpd-14-32935-2014.

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Abstract. Recent work has demonstrated that organic and mixed organic–inorganic particles can exhibit multiple phase states depending on their chemical composition and on ambient conditions such as relative humidity (RH). To explore the extent to which water uptake varies with particle phase behavior, hygroscopic growth factors (HGFs) of nine laboratory-generated, organic and organic–inorganic aerosol systems with physical states ranging from well-mixed liquids, to phase-separated particles, to viscous liquids or semi-solids were measured with the Differential Aerosol Sizing and Hygroscopicity

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19

Hodas, N., A. Zuend, W. Mui, R. C. Flagan, and J. H. Seinfeld. "Influence of particle-phase state on the hygroscopic behavior of mixed organic–inorganic aerosols." Atmospheric Chemistry and Physics 15, no. 9 (2015): 5027–45. http://dx.doi.org/10.5194/acp-15-5027-2015.

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Abstract. Recent work has demonstrated that organic and mixed organic–inorganic particles can exhibit multiple phase states depending on their chemical composition and on ambient conditions such as relative humidity (RH). To explore the extent to which water uptake varies with particle-phase behavior, hygroscopic growth factors (HGFs) of nine laboratory-generated, organic and organic–inorganic aerosol systems with physical states ranging from well-mixed liquids to phase-separated particles to viscous liquids or semi-solids were measured with the Differential Aerosol Sizing and Hygroscopicity S

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20

Yue, Xu Dong, Guang Can Jin, Shu Ying Chen та Guo Wei Chang. "In Situ Observation of Growth Process of δ Phase of 0.15% C Carbon Steel during Solidification". Advanced Materials Research 299-300 (липень 2011): 341–44. http://dx.doi.org/10.4028/www.scientific.net/amr.299-300.341.

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In situ observation of growth process of high temperature phase in 0.15% C carbon steel during solidification concerned with using Confocal Scanning Laser Microscope (CSLM), the growth rate of -phase has been measured. The results indicate that high temperature -phase grows at cell crystal way when the cooling speed reaches 2°C/min in 0.15% C carbon steel. The -phase of round or oval cross-sectional shaped may grow stably. The growth rate of -phase is gradually getting slow along with increasing of curvature radius. The variation of growth speed tends to be similar with different solid-liquid

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21

Орешкин, В. И. "Рост перегревных неустойчивостей в метастабильном металле". Письма в журнал технической физики 44, № 20 (2018): 62. http://dx.doi.org/10.21883/pjtf.2018.20.46807.17432.

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AbstractThe development of thermal (overheat) instabilities during the electric explosion of a conducting wire has been analyzed using the theory of small perturbations. At the initial stage of electric explosion (upon melting of the metal), the substance can occur in three phases: liquid, two-phase state (liquid + vapor), and metastable metal liquid (overheated liquid). Comparative analysis of the growth of overheat instabilities is performed as dependent on the phase in which the metal can occur. It is shown that, from the standpoint of development of overheat instability, the most unstable

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22

Fornaro, Osvaldo. "Directional Solidification of Sn-Cu6Sn5 In Situ Composites." Advances in Materials Science and Engineering 2019 (March 13, 2019): 1–8. http://dx.doi.org/10.1155/2019/9210713.

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The Sn-Cu system presents an important interest from academic and technological point of view because it is part of the family of alloys proposed as lead-free solder alloys for electronic components and also due to the mechanisms involved during the growth of the different phases. Sn-Cu system has two intermetallic phases, i.e., ε-Cu3Sn and η-Cu6Sn5, and η can be used as the negative (anode) electrode in Li-ion batteries, alone or as part of (Co,Ni)xCu6−xSn5-type composites. Obtaining this η phase from liquid with the appropriate chemical composition is a very difficult task because it has a f

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23

Dong, C., J. M. Dubois, M. de Boissieu, M. Boudard, and C. Janot. "Growth of stable Al–Pd–Mn icosahedral phase." Journal of Materials Research 6, no. 12 (1991): 2637–45. http://dx.doi.org/10.1557/jmr.1991.2637.

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We have carried out a detailed investigation of the Al71Pd19Mn10 alloy by using a combination of experimental techniques (neutron diffraction, electron diffraction, high resolution electron microscopy, and electron probe microanalysis). This alloy contains only the perfect icosahedral phase. This icosahedral phase is stable from room temperature up to its melting, though a transient cubic metastable phase coexists with it during the heating. It grows directly from liquid without involving any crystalline phase. Its isothermal growths at different temperatures can well be described by the Avram

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24

Wołczyński, Waldemar. "Concentration Micro-Field for Lamellar Eutectic Growth." Defect and Diffusion Forum 272 (March 2008): 123–38. http://dx.doi.org/10.4028/www.scientific.net/ddf.272.123.

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A possibility of a modification of the Jackson-Hunt theory of an oriented structure formation is analysed. A new model for the formation of a concentration field ahead of growing regular lamellae with respect to the solid / liquid interface shape is presented. A coordinate system applied in the model is attached to the solid / liquid interface to be advancing in the z - direction, identically with interface moving at a constant velocity, v . The solution to a diffusion equation is given for the improved formulation of the boundary conditions. The boundary conditions are related to the interpla

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25

Gautam, S. K., and S. P. Gupta. "Kinetics of the discontinuous precipitation of a liquid phase in Cu–In alloys." International Journal of Materials Research 94, no. 11 (2003): 1247–54. http://dx.doi.org/10.1515/ijmr-2003-0225.

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Abstract The morphology and growth kinetics of the discontinuous precipitation of liquid and depleted solid phases from a supersaturated solid solution has been studied. The transformation was carried out in the two-phase (liquid + solid α) field in the temperature range 996–1050 K in two Cu– In alloys containing 8.9 and 9.5 at.% In. A lamellar structure consisting of alternate lamellae of α and liquid phases has been observed to grow from the grain boundaries of the supersaturated α solid solution. The nucleation of the liquid droplets occurred at the grain boundary and a thin layer of liquid

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26

Liu, Dan, Yong Ke Yan, and He Ping Zhou. "Effect of PbO Concentration on the Templated Grain Growth of PMN-32.5PT Ceramics." Key Engineering Materials 368-372 (February 2008): 15–17. http://dx.doi.org/10.4028/www.scientific.net/kem.368-372.15.

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<001> textured 0.675Pb(Mg1/3Nb2/3)O3-0.325PbTiO3 (PMN-32.5PT) ceramics were prepared by templated grain growth with micron scale BaTiO3 platelet templates. 0%~7% excess PbO was added to form liquid phase. The influence of liquid phase concentration on the growth of matrix and templated grains was investigated. The growth process was controlled by a dissolution-precipitation mechanism. The templated grain growth was accelerated by the formed liquid phase and resulted in highly textured PMN-32.5PT ceramics.

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27

HU, Shu-Hong, Feng QIU, Ying-Fei LV, et al. "GaSb Quantum Dots growth by Liquid Phase Epitaxy." Journal of Infrared and Millimeter Waves 32, no. 3 (2013): 220. http://dx.doi.org/10.3724/sp.j.1010.2013.00220.

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28

PEZZOTTI, Giuseppe, Hans-Joachim KLEEBE, Toshihiko NISHIDA, and Günter ZIEGLER. "Growth Isotherms of Liquid-Phase Sintered Silicon Nitride." Journal of the Ceramic Society of Japan 105, no. 1224 (1997): 638–40. http://dx.doi.org/10.2109/jcersj.105.638.

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29

NISHITANI-GAMO, Mikka, Kiyoharu NAKAGAWA, Yafei ZHANG, Keishin OTA, Hidenori GAMO, and Toshihiro ANDO. "Liquid Phase Growth of Carbon Nanotubes in Alcohols." Journal of the Surface Finishing Society of Japan 53, no. 12 (2002): 915–19. http://dx.doi.org/10.4139/sfj.53.915.

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30

Laxmanan, V. "Dendritic growth during liquid to solid phase transitions." Physical Review E 57, no. 2 (1998): 2004–9. http://dx.doi.org/10.1103/physreve.57.2004.

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31

He, Chengyu, Xizhang Wang, Qiang Wu, et al. "Phase-Equilibrium-Dominated Vapor−Liquid−Solid Growth Mechanism." Journal of the American Chemical Society 132, no. 13 (2010): 4843–47. http://dx.doi.org/10.1021/ja910874x.

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32

Amano, Toshimasa, Susumu Kondo, and Haruo Nagai. "High Purity Liquid Phase Epitaxial Growth of InP." Japanese Journal of Applied Physics 32, Part 1, No. 11A (1993): 4878–84. http://dx.doi.org/10.1143/jjap.32.4878.

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33

Kursumovic, A., R. I. Tomov, R. Hühne, J. L. MacManus-Driscoll, B. A. Glowacki, and J. E. Evetts. "Hybrid liquid phase epitaxy processes for YBa2Cu3O7film growth." Superconductor Science and Technology 17, no. 10 (2004): 1215–23. http://dx.doi.org/10.1088/0953-2048/17/10/024.

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34

Chang, L. B., K. Y. Cheng, and C. C. Liu. "Magnesium‐doped In0.5Ga0.5P growth by liquid‐phase epitaxy." Journal of Applied Physics 64, no. 3 (1988): 1116–19. http://dx.doi.org/10.1063/1.341870.

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35

Lyubimov, D. V., T. P. Lyubimova, S. Meradji, and B. Roux. "Vibrational control of crystal growth from liquid phase." Journal of Crystal Growth 180, no. 3-4 (1997): 648–59. http://dx.doi.org/10.1016/s0022-0248(97)00294-7.

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36

Yongzhen, Wang, Jin Changchun, and Lu Guijin. "Liquid-phase epitaxial growth of InAsPSb/InAs heterostructure." Journal of Crystal Growth 187, no. 2 (1998): 194–96. http://dx.doi.org/10.1016/s0022-0248(97)00872-5.

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37

Yamaguchi, Toshinao, Fumito Ueda, and Masaaki Imamura. "Growth of Superconductive Bi2Sr2CaCu2OxFilm by Liquid Phase Epitaxy." Japanese Journal of Applied Physics 32, Part 1, No. 4 (1993): 1634–35. http://dx.doi.org/10.1143/jjap.32.1634.

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38

Amano, Toshimasa, Susumu Kondo, Haruo Nagai, and Susumu Maruyama. "Ultrahigh Purity Liquid Phase Epitaxial Growth of GaAs." Japanese Journal of Applied Physics 32, Part 1, No. 9A (1993): 3692–99. http://dx.doi.org/10.1143/jjap.32.3692.

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39

Syväjärvi, M., R. Yakimova, and E. Janzén. "Interfacial Properties in Liquid Phase Growth of SiC." Journal of The Electrochemical Society 146, no. 4 (1999): 1565–69. http://dx.doi.org/10.1149/1.1391805.

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40

Hiura, Hidefumi, Michael V. Lee, Anastasia V. Tyurnina, and Kazuhito Tsukagoshi. "Liquid phase growth of graphene on silicon carbide." Carbon 50, no. 14 (2012): 5076–84. http://dx.doi.org/10.1016/j.carbon.2012.06.047.

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41

Logan, R. A. "Liquid phase epitaxial growth of buried heterostructure devices." Journal of Crystal Growth 83, no. 2 (1987): 233–37. http://dx.doi.org/10.1016/0022-0248(87)90012-1.

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42

Bryskiewicz, T., C. F. Boucher, J. Lagowski, and H. C. Gatos. "Bulk GaAs crystal growth by liquid phase electroepitaxy." Journal of Crystal Growth 82, no. 3 (1987): 279–88. http://dx.doi.org/10.1016/0022-0248(87)90315-0.

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43

Tew, Bo E., Matthew R. Lewis, Chun-Yen Hsu, Chaoying Ni, and Joshua M. O. Zide. "Growth of ErAs:GaAs nanocomposite by liquid phase epitaxy." Journal of Crystal Growth 518 (July 2019): 34–38. http://dx.doi.org/10.1016/j.jcrysgro.2019.04.025.

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44

Lazzari, J. L., J. L. Leclercq, P. Grunberg, et al. "Liquid phase epitaxial growth of AlGaAsSb on GaSb." Journal of Crystal Growth 123, no. 3-4 (1992): 465–78. http://dx.doi.org/10.1016/0022-0248(92)90608-l.

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45

Takemoto, J., S. Miyashita, T. Inoue, and H. Komatsu. "Liquid phase epitaxial growth of bismuth based superconductors." Journal of Crystal Growth 163, no. 1-2 (1996): 100–104. http://dx.doi.org/10.1016/0022-0248(95)01041-6.

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46

Lu, Yanli, Yingying Peng, and Zheng Chen. "A binary phase field crystal study for liquid phase heteroepitaxial growth." Superlattices and Microstructures 97 (September 2016): 132–39. http://dx.doi.org/10.1016/j.spmi.2016.05.039.

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47

Park, Sang Yeup, Jun Ho Song, and Young Jin Cho. "Effect of Grain Orientation on the Abnormal Grain Growth with Magetoplumbite Crystal Structure." Materials Science Forum 558-559 (October 2007): 1265–70. http://dx.doi.org/10.4028/www.scientific.net/msf.558-559.1265.

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The nucleation and growth behavior of magentoplombite has been observed during the abnormal grain growth in the presence of liquid phase. Abnormal grain growth was explained in terms of grain orientation due to liquid phase. It has been observed that the nuclei formation for abnormal grain growth was driven by the capillary force due to the liquid phase. Because magnetoplumbite crystal structure has an anisotropic crystal nature, abnormal grain growth with faceted grain shape was observed depending on its chemical composition. The formation of nuclei and particle orientation was important for

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48

Renbaum-Wolff, L., M. Song, C. Marcolli та ін. "Observations and implications of liquid–liquid phase separation at high relative humidities in secondary organic material produced by α-pinene ozonolysis without inorganic salts". Atmospheric Chemistry and Physics Discussions 15, № 22 (2015): 33379–405. http://dx.doi.org/10.5194/acpd-15-33379-2015.

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Abstract. Particles consisting of secondary organic material (SOM) are abundant in the atmosphere. To predict the role of these particles in climate, visibility, and atmospheric chemistry, information on particle phase state (i.e. single liquid, two liquids, solid and so forth) is needed. This paper focuses on the phase state of SOM particles free of inorganic salts produced by the ozonolysis of α-pinene. Phase transitions were investigated both in the laboratory and with a thermodynamic model over the range of < 0.5 % to 100 % relative humidity (RH) at 290 K. In the laboratory studies, a s

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49

Talbot, Emma L., Jurij Kotar, Lorenzo Di Michele, and Pietro Cicuta. "Directed tubule growth from giant unilamellar vesicles in a thermal gradient." Soft Matter 15, no. 7 (2019): 1676–83. http://dx.doi.org/10.1039/c8sm01892h.

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We demonstrate experimental control over tubule growth in giant unilamellar vesicles with liquid–liquid phase coexistence, using a thermal gradient to redistribute lipid phase domains on the membrane.

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50

Feng, Li, Ling Min An, Chang Sheng Zhu, Yang Lu, Rong Zhen Xiao, and Bo Cheng. "Phase-Field Simulation Studies of Multiple Grains Coupled with Force Flow Field." Advanced Materials Research 915-916 (April 2014): 1038–48. http://dx.doi.org/10.4028/www.scientific.net/amr.915-916.1038.

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Coupling the force flow field with the phase field model for the isothermal growth of dendrite multiple grains, Sola algorithm is used to calculate the flow speed and pressure of liquid metal, double grid numerical method was used to reduce the calculation amount of computer simulation, the space factor and time factor were introduced to improve the accuracy of double grid numerical calculation, Taking Al-2%-Cu alloy for example, the dendrite growth process of the binary alloy was simulated under forced convection environment; Simulation results can capture the real dendrite growth and interac

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