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Journal articles on the topic 'Congruent melting'

Author: Grafiati
Published: 4 June 2021
Last updated: 11 February 2022

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1

Huang, Shuzhao, Chen Zhou, Shichao Cheng, and Feng Yu. "K5B19O31: A Deep‐Ultraviolet Congruent Melting Compound." ChemistrySelect 4, no. 35 (September 17, 2019): 10436–41. http://dx.doi.org/10.1002/slct.201902453.

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2

Greenwood, James P., and Paul C. Hess. "Congruent melting kinetics of albite: Theory and experiment." Journal of Geophysical Research: Solid Earth 103, B12 (December 10, 1998): 29815–28. http://dx.doi.org/10.1029/98jb02300.

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3

Hao, Wenyu, Yemao Han, Rongjin Huang, Kai Feng, Wenlong Yin, Jiyong Yao, and Yicheng Wu. "Ag1.75InSb5.75Se11: A new noncentrosymmetric compound with congruent-melting behavior." Journal of Solid State Chemistry 218 (October 2014): 196–201. http://dx.doi.org/10.1016/j.jssc.2014.06.026.

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4

Yao, Jiyong, Dajiang Mei, Lei Bai, Zheshuai Lin, Wenlong Yin, Peizhen Fu, and Yicheng Wu. "BaGa4Se7: A New Congruent-Melting IR Nonlinear Optical Material." Inorganic Chemistry 49, no. 20 (October 18, 2010): 9212–16. http://dx.doi.org/10.1021/ic1006742.

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5

Kunieda, H., H. Ito, S. Takebayashi, and M. Kodama. "Azeotropic-like (congruent melting) phenomena of lamellar liquid crystals." Colloid & Polymer Science 271, no. 10 (October 1993): 952–59. http://dx.doi.org/10.1007/bf00654855.

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6

Glew, David N. "Aqueous nonelectrolyte solutions — Part XX: Formula of structure I methane hydrate, congruent dissociation melting point, and formula of the metastable hydrate." Canadian Journal of Chemistry 81, no. 12 (December 1, 2003): 1443–50. http://dx.doi.org/10.1139/v03-156.

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Sixteen new measurements of high precision for structure I methane hydrate with water between 31.93 and 47.39 °C are shown to be metastable and exhibit higher methane pressures than found by earlier workers. Comparison of earlier measurements between 26.7 and 47.2 °C permit positive identification of the structure II and the structure I hydrates. Forty-nine equilibrium constants Kp(h1[Formula: see text]l1g) for dissociation of structure I methane hydrate into water and methane, 32 between –0.29 and 26.7 °C for the stable hydrate and 17 between 31.93 and 47.39 °C for the metastable hydrate, are best represented by a three-parameter thermodynamic equation, which indicates a standard error (SE) of 0.63% on a single Kp(h1[Formula: see text]l1g) determination. The congruent dissociation melting point C(h1l1gxm) of metastable structure I methane hydrate is at 47.41 °C with SE 0.02 °C and at pressure 505 MPa. The congruent equilibrium constant Kp(h1[Formula: see text]l1g) is 102.3 MPa with SE 0.2 MPa. ΔH°t(h1[Formula: see text]l1g) is 62 281 J mol–1 with SE 184 J mol–1, and the congruent formula is CH4·5.750H2O with SE 0.059H2O. At the congruent point, ΔV(h1[Formula: see text]l1g) is zero within experimental precision, and its estimate is 1.3 with SE 1.6 cm3 mol–1. The stability range of structure I methane hydrate with water extends from quadruple point Q(s1h1l1g) at –0.29 °C up to quadruple point Q(h1h2l1g) at 26.7 °C, and its metastability range with water extends from 26.7 °C up to the congruent dissociation melting point C(h1l1gxm) at 47.41 °C. Key words: methane hydrate, clathrate structure I, metastability range, dissociation equilibrium constant, formula, congruent melting point, metastability of structure I hydrate.
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7

White, Mary Anne, and Randall T. Perry. "Melting Behavior in Binary Compounds: Inclusion Compounds as Examples of Congruent vs Incongruent Melting." Chemistry of Materials 6, no. 5 (May 1994): 603–10. http://dx.doi.org/10.1021/cm00041a008.

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8

Welland, M. J., W. T. Thompson, B. J. Lewis, and D. Manara. "Computer simulations of non-congruent melting of hyperstoichiometric uranium dioxide." Journal of Nuclear Materials 385, no. 2 (March 2009): 358–63. http://dx.doi.org/10.1016/j.jnucmat.2008.12.023.

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9

Dong, Xiaoyu, Liang Cui, Yunjing Shi, Shilie Pan, Zhongxiang Zhou, Zhihua Yang, Bingbing Zhang, et al. "Ba2Cd(B3O6)2: A Congruent-Melting Compound with Isolated B3O6Units." Zeitschrift für anorganische und allgemeine Chemie 639, no. 6 (April 26, 2013): 988–93. http://dx.doi.org/10.1002/zaac.201300047.

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10

Rouland, J. C., S. Makki, J. L. Fournival, and R. Céolin. "Congruent melting of binary compounds with non-negligible vapour pressure." Journal of Thermal Analysis 45, no. 6 (December 1995): 1507–23. http://dx.doi.org/10.1007/bf02547444.

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11

Rouland, J. C., A. Thorén, J. L. Fournival, and R. Céolin. "Congruent melting of binary compounds with non-negligible vapour pressure." Journal of Thermal Analysis 44, no. 6 (June 1995): 1417–37. http://dx.doi.org/10.1007/bf02549229.

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12

Vinnik, D. A., M. V. Sudarikov, and V. E. Zhivulin. "Experimental Study of Ba7Fe4O13, Ba3Fe2O6, Ba2Fe2O5, BaFe2O4 Barium Ferrites." Materials Science Forum 870 (September 2016): 70–73. http://dx.doi.org/10.4028/www.scientific.net/msf.870.70.

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This paper presents the results of synthesis of BaO-Fe2O3 system compounds. The powder X-ray diffraction patterns are presented. The patterns of Ba3Fe2O6, Ba2Fe2O5 and BaFe2O4 coincide with literature data. The experimental cell parameters were calculated. The study results of nature and the melting temperatures of Ba3Fe2O6, Ba7Fe4O13, Ba2Fe2O5, BaFe2O4 are described. The compounds have congruent melting character. The melting temperatures of listed compounds are 1325, 1320, 1365, 1405 °C (1598, 1593, 1638, 1678 K), respectively.
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13

Glew, David N. "Aqueous nonelectrolyte solutions. Part XIX. Congruent dissociation melting point and the formula of structure II methane hydrate." Canadian Journal of Chemistry 81, no. 2 (February 1, 2003): 179–85. http://dx.doi.org/10.1139/v03-004.

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Twenty-four equilibrium pressures, P(h2l1g), of structure II methane hydrate h2 with water l1 between 27.0 and 46.9°C are well represented by a four-parameter equation, which indicates a standard error (SE) of 1.95% on a single pressure measurement. Forty equilibrium constants Kp(h2[Formula: see text]l1g) for dissociation of structure II methane hydrate into water and methane between 27.0 and 47.7°C and at pressures up to 784 MPa at 45.0°C are best represented by a three-parameter thermodynamic equation, which indicates an SE 1.25% on a single Kp(h2[Formula: see text]l1g) determination. The congruent dissociation melting point C(h2l1gxm) of structure II methane hydrate is at 47.71°C with SE 0.03°C and at pressure 533 MPa with SE 5 MPa. The congruent Kp(h2[Formula: see text]l1g) is 102.9 with SE 0.3 MPa, ΔH°t(h2[Formula: see text]l1g) is 61 531 with SE 244 J mol–1, and the congruent formula is CH4·5.670H2O with SE 0.061H2O. At congruent point ΔV(h2[Formula: see text]l1g) = 0 and its estimate is 1.0 with SE 1.6 cm3 mol–1. Stability range of structure II methane hydrate with water extends from quadruple point Q(h1h2l1g) at 26.7°C and 55.5 MPa up to quadruple point Q(h2h3l1g) at 47.3°C and 620 MPa. The metastability range of structure I methane hydrate with water is discussed.Key words: methane hydrate, clathrate structure II, stability range, dissociation equilibrium constant, formula, congruent melting point, metastability of structure I hydrate.
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14

Xing, Wenhao, Naizheng Wang, Yangwu Guo, Zhuang Li, Jian Tang, Kaijin Kang, Wenlong Yin, Zheshuai Lin, Jiyong Yao, and Bin Kang. "Two rare-earth-based quaternary chalcogenides EuCdGeQ4 (Q = S, Se) with strong second-harmonic generation." Dalton Transactions 48, no. 47 (2019): 17620–25. http://dx.doi.org/10.1039/c9dt03755a.

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Two RE-based quaternary metal chalcogenides EuCdGeQ4 (Q = S, Se) are discovered. They possess many attractive properties as preferred IR NLO materials including large band gaps, phase-matched intense SHG and congruent melting behavior.
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15

Pustovgar, E. A., S. N. Igumnov, M. A. Kiskin, and I. A. Uspenskaya. "Structure and properties of congruent melting 18-crown-6 crystalline hydrates." Thermochimica Acta 510, no. 1-2 (October 2010): 154–59. http://dx.doi.org/10.1016/j.tca.2010.07.009.

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16

Li, Feng, Xueling Hou, Shilie Pan, and Xian Wang. "Growth, Structure, and Optical Properties of a Congruent Melting Oxyborate, Bi2ZnOB2O6." Chemistry of Materials 21, no. 13 (July 14, 2009): 2846–50. http://dx.doi.org/10.1021/cm900560x.

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17

Yao, Jiyong, Dajiang Mei, Lei Bai, Zheshuai Lin, Wenlong Yin, Peizhen Fu, and Yicheng Wu. "ChemInform Abstract: BaGa4Se7: A New Congruent-Melting IR Nonlinear Optical Material." ChemInform 41, no. 50 (November 18, 2010): no. http://dx.doi.org/10.1002/chin.201050014.

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18

Hao, Wenyu, Yemao Han, Rongjin Huang, Kai Feng, Wenlong Yin, Jiyong Yao, and Yicheng Wu. "ChemInform Abstract: Ag1.75InSb5.75Se11: A New Noncentrosymmetric Compound with Congruent-Melting Behavior." ChemInform 45, no. 41 (September 25, 2014): no. http://dx.doi.org/10.1002/chin.201441023.

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19

Nianyi, Chen, Li Chonghe, Yao Shuwen, and Wang Xueye. "Regularities of melting behavior of some binary alloy phases. Part 1. Criteria for congruent and incongruent melting." Journal of Alloys and Compounds 234, no. 1 (February 1996): 125–29. http://dx.doi.org/10.1016/0925-8388(95)01962-6.

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20

Futami, Yoshisuke, Yuui Yokota, Masato Sato, Kazushige Tota, Jan Pejchal, Takayuki Yanagida, Ko Onodera, and Akira Yoshikawa. "Study on Phase Diagram of Ca3NbGa3Si2O14 Piezoelectric Material by Differential Thermal Analysis and X-Ray Diffraction Measurement." Key Engineering Materials 508 (March 2012): 247–52. http://dx.doi.org/10.4028/www.scientific.net/kem.508.247.

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Ca3NbGa3Si2O14 (CNGS) Is One of the Langasite-Type Crystals and it Is Known as a Piezoelectric Material. We Have Successfully Grown the Shaped CNGS Crystal Using Micro-Pulling-down (μ-PD) Method with Shape Control. However, the Impurity Phases such as Ca-Nb-O Related Compounds Were Detected in the Grown Crystals. The Creation of the Impurity Phases Is Related to Difference in Stoichiometric and Congruent Compositions. Therefore, the Detailed Investigation of Phase Diagram on CNGS Was Carried Out to Prevent the Impurity Phases Creation. It Follows from the TG-DTA Measurements that the Melting Point Systematically Changed with the Ca/Ga Ratio in the Ca3-xNbGa3+xSi2O14±δ Cmpositions. The CNGS Phase with Ca/Ga = 1.02 Indicated the Maximum Melting Point which Suggests that the Stoichiometric Composition of CNGS Is Different in the Congruent Composition. Furthermore, in the DTA Measurements the Peaks of Impurity Phases Were Detected around 1550 °C for the CNGS Sample with Ca/Ga = 1.02.
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21

Bulina, Natalia V., Sergey G. Baev, Svetlana V. Makarova, Alexander M. Vorobyev, Alexander I. Titkov, Victor P. Bessmeltsev, and Nikolay Z. Lyakhov. "Selective Laser Melting of Hydroxyapatite: Perspectives for 3D Printing of Bioresorbable Ceramic Implants." Materials 14, no. 18 (September 19, 2021): 5425. http://dx.doi.org/10.3390/ma14185425.

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Hydroxyapatite, being the major mineral component of tooth enamel and natural bones, is a good candidate for bone tissue engineering applications. One of the promising approaches for manufacturing of three-dimensional objects is selective laser sintering/melting which enables the creation of a dense structure directly during 3D printing by adding material layer-by-layer. The effect of laser irradiation with a wavelength of 10.6 μm on the behavior of mechanochemically synthesized hydroxyapatite under different treatment conditions was studied for the first time in this work. It was shown that, in contrast to laser treatment, the congruent melting is impossible under conditions of a relatively slow rate of heating in a furnace. Depending on the mode of laser treatment, hydroxyapatite can be sintered or melted, or partially decomposed into the more resorbable calcium phosphates. It was found that the congruent selective laser melting of hydroxyapatite can be achieved by treating the dense powder layer with a 0.2 mm laser spot at a power of 4 W and at a scanning speed of 700 mm/s. Melting was shown to be accompanied by the crystallization of a dense monolayer of oxyhydroxyapatite while preserving the initial apatite crystal lattice. The thickness of the melted layer, the presence of micron-sized pores, and the phase composition can be controlled by varying the scanning speed and laser power. This set of parameters permits the use of selective laser melting technology for the production of oxyhydroxyapatite biodegradable implants with acceptable properties by 3D printing.
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22

Dou, Yunwei, Ying Chen, Zhuang Li, Abishek K. Iyer, Bin Kang, Wenlong Yin, Jiyong Yao, and Arthur Mar. "SrCdGeS4 and SrCdGeSe4: Promising Infrared Nonlinear Optical Materials with Congruent-Melting Behavior." Crystal Growth & Design 19, no. 2 (January 7, 2019): 1206–14. http://dx.doi.org/10.1021/acs.cgd.8b01649.

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23

Zhou, Zhongxiang, and et al et al. "ChemInform Abstract: Ba2Cd(B3O6)2: A Congruent-Melting Compound with Isolated B3O6Units." ChemInform 44, no. 30 (July 4, 2013): no. http://dx.doi.org/10.1002/chin.201330003.

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24

Mukhanov, Vladimir A., Petr S. Sokolov, Andrey N. Baranov, Victor Yu Timoshenko, Denis M. Zhigunov, and Vladimir L. Solozhenko. "Congruent melting and rapid single-crystal growth of ZnO at 4 GPa." CrystEngComm 15, no. 32 (2013): 6318. http://dx.doi.org/10.1039/c3ce40766g.

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25

Schroer, J. W., and P. A. Monson. "Understanding congruent melting in binary solids: Molecular models of benzene–hexafluorobenzene mixtures." Journal of Chemical Physics 118, no. 6 (2003): 2815. http://dx.doi.org/10.1063/1.1531586.

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26

Zhou, Molin, Xingxing Jiang, Mingjun Xia, Hongwei Huang, Zheshuai Lin, Jiyong Yao, and Yicheng Wu. "A new congruent-melting double phosphate PbCd(PO3)4 with photocatalytic activity." Journal of Alloys and Compounds 689 (December 2016): 599–605. http://dx.doi.org/10.1016/j.jallcom.2016.08.011.

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27

Zhuang, Naifeng, Wenbing Chen, Lijun Shi, Jianbiao Nie, Xiaolin Hu, Bin Zhao, Shukun Lin, and Jianzhong Chen. "A new technique to grow incongruent melting Ga:YIG crystals: the edge-defined film-fed growth method." Journal of Applied Crystallography 46, no. 3 (May 15, 2013): 746–51. http://dx.doi.org/10.1107/s002188981301025x.

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Crystalline yttrium iron garnet (YIG) is an important magneto-optical material. However, this crystal is an incongruent melting compound. As is well known, compared to the crystal growth of a congruent melting compound by using the Czochralski method, the crystal growth of an incongruent melting compound is more difficult. In this work, a system for growing Ga:YIG single crystals by the edge-defined film-fed growth (EFG) method was designed and constructed, and the mechanism of crystal growth was also preliminarily studied. The Ga3+dopant concentration, the Curie temperature and the transmission spectra of as-grown crystals were investigated to evaluate their potential application in magneto-optical devices. The success of growing Ga:YIG crystals by the EFG method provides a new way to grow other incongruent melting compounds.
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28

Brandle, C. D., and V. J. Fratello. "Preparation of perovskite oxides for high Tc superconductor substrates." Journal of Materials Research 5, no. 10 (October 1990): 2160–64. http://dx.doi.org/10.1557/jmr.1990.2160.

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A variety of materials of the general type A2BB′O6 that have an ordered perovskite structure have been prepared and examined as possible substrate candidates for high Tc superconducting films. Materials containing either Ca or Sr as the A cation and either Ga or Al in combination with Nb or Ta as the B and B′ cations have been shown to be congruent melting compounds. These compounds have melting points easily accessible using conventional rf heating techniques and are therefore materials that could possibly be grown in bulk form using the Czochralski growth technique.
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29

Parameshwaran, Rajagolalan, and Siva Kalaiselvam. "Thermal Energy Storage Properties of Hybrid Nanocomposite – Embedded Phase Change Material for Sustainable Buildings." Advanced Materials Research 935 (May 2014): 251–54. http://dx.doi.org/10.4028/www.scientific.net/amr.935.251.

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The thermal properties of the new copper–titania hybrid nanocomposite embedded organic ester phase change material (HNPCM) were analyzed experimentally. The surface functionalized hybrid nanocomposite (HyNC) embedded into the PCM has effectively created the densely packed network of thermal interfaces in the PCM matrix layers. The experimental results suggest that, the incorporation of the HyNC has enabled the HNPCM to exhibit improved thermal conductivity (0.347 W/m K), congruent phase transition temperature (freezing: 33.53ᵒC, melting: 35.32 ᵒC), high latent heat capacity (freezing: 109.05 kJ/kg, melting: 109.14 kJ/kg) and considerable reduction in (freezing time: 21.2%, melting time: 29.2%). The improved thermal properties being achieved facilitate the HNPCM to be considered as a viable thermal storage material for high performance and sustainable building cooling and heating applications.
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30

Ott, J. Bevan, and J. Rex Goates. "Summary of Melting and Transition Temperatures of Pure Substances and Congruent and Incongruent Melting Temperatures of Molecular Addition Compounds." Journal of Chemical & Engineering Data 41, no. 4 (January 1996): 669–77. http://dx.doi.org/10.1021/je9601063.

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31

Wang, Shou-Qi, Jiro Harada, and Satoshi Uda. "Study of congruent-melting composition of langasite and its effects on crystal quality." Journal of Crystal Growth 219, no. 3 (October 2000): 263–68. http://dx.doi.org/10.1016/s0022-0248(00)00620-5.

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32

Luo, Xiaoyu, Fei Liang, Molin Zhou, Yangwu Guo, Zhuang Li, Zheshuai Lin, Jiyong Yao, and Yicheng Wu. "K2ZnGe3S8: A Congruent-Melting Infrared Nonlinear-Optical Material with a Large Band Gap." Inorganic Chemistry 57, no. 15 (July 13, 2018): 9446–52. http://dx.doi.org/10.1021/acs.inorgchem.8b01437.

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33

Li, Hongyi, Yi Zhao, Shilie Pan, Hongping Wu, Hongwei Yu, Fangfang Zhang, Zhihua Yang, and Kenneth R. Poeppelmeier. "Synthesis and Structure of KPbBP2O8- A Congruent Melting Borophosphate with Nonlinear Optical Properties." European Journal of Inorganic Chemistry 2013, no. 18 (May 10, 2013): 3185–90. http://dx.doi.org/10.1002/ejic.201300009.

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34

Fujii, Shunsuke, Satoshi Uda, Kensaku Maeda, Jun Nozawa, Haruhiko Koizumi, Kozo Fujiwara, and Tomio Kajigaya. "Growth of congruent-melting lithium tantalate crystal with stoichiometric structure by MgO doping." Journal of Crystal Growth 383 (November 2013): 63–66. http://dx.doi.org/10.1016/j.jcrysgro.2013.08.020.

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35

Roland, C. Michael, and Gary S. Buckley. "Thermal Crystallization of Polytetrahydrofuran Networks." Rubber Chemistry and Technology 64, no. 1 (March 1, 1991): 74–82. http://dx.doi.org/10.5254/1.3538542.

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Abstract The formation of a network in PTHF inhibits the crystallization of chain units in proximity to the crosslinks. From melting-point-depression measurements, it is estimated that the suppression in crystallizability extends to as much as 8 chain units away from a network junction. This estimate is consistent with the degree of crystallinity measured in various crosslinked PTHF rubbers. The equilibrium melting point for linear PTHF was determined to be 361°K. Although this is significantly higher than previously reported values, the present result is congruent with the melting temperatures measured for crosslinked PTHF, and its use leads to satisfactory predictions of their melting-point depression. The distribution in the lengths of network chains exerted a trivial influence on thermal crystallization behavior. Although this distribution must in principle influence crystallization behavior in so far as it governs crystallizable sequence lengths, differences between uni- and bi-modal network architectures were moderate under the present experimental conditions.
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36

Tournier, Robert F., and Michael I. Ojovan. "Building and Breaking Bonds by Homogenous Nucleation in Glass-Forming Melts Leading to Transitions in Three Liquid States." Materials 14, no. 9 (April 28, 2021): 2287. http://dx.doi.org/10.3390/ma14092287.

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The thermal history of melts leads to three liquid states above the melting temperatures Tm containing clusters—bound colloids with two opposite values of enthalpy +Δεlg × ΔHm and −Δεlg × ΔHm and zero. All colloid bonds disconnect at Tn+ > Tm and give rise in congruent materials, through a first-order transition at TLL = Tn+, forming a homogeneous liquid, containing tiny superatoms, built by short-range order. In non-congruent materials, (Tn+) and (TLL) are separated, Tn+ being the temperature of a second order and TLL the temperature of a first-order phase transition. (Tn+) and (TLL) are predicted from the knowledge of solidus and liquidus temperatures using non-classical homogenous nucleation. The first-order transition at TLL gives rise by cooling to a new liquid state containing colloids. Each colloid is a superatom, melted by homogeneous disintegration of nuclei instead of surface melting, and with a Gibbs free energy equal to that of a liquid droplet containing the same magic atom number. Internal and external bond number of colloids increases at Tn+ or from Tn+ to Tg. These liquid enthalpies reveal the natural presence of colloid–colloid bonding and antibonding in glass-forming melts. The Mpemba effect and its inverse exist in all melts and is due to the presence of these three liquid states.
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37

Xia, M. J., and R. K. Li. "Crystal structure, growth and characterization of LiPbB9O15: A new congruent melting nonlinear optical crystal." Journal of Solid State Chemistry 201 (May 2013): 288–92. http://dx.doi.org/10.1016/j.jssc.2013.03.001.

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38

Fedorov, P. P., and Irina I. Buchinskaya. "Spatial inhomogeneity in crystalline materials and saddle-type congruent melting points in ternary systems." Russian Chemical Reviews 81, no. 1 (January 31, 2012): 1–20. http://dx.doi.org/10.1070/rc2012v081n01abeh004207.

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39

Wang, Xuefei, Ying Wang, Bingbing Zhang, Fangfang Zhang, Zhihua Yang, and Shilie Pan. "CsB4O6F: A Congruent-Melting Deep-Ultraviolet Nonlinear Optical Material by Combining Superior Functional Units." Angewandte Chemie International Edition 56, no. 45 (October 4, 2017): 14119–23. http://dx.doi.org/10.1002/anie.201708231.

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40

Guo, Xinfeng, Hongping Wu, Shilie Pan, Zhihua Yang, Hongwei Yu, Bingbing Zhang, Jian Han, and Fangyuan Zhang. "Synthesis, Crystal Structure, and Characterization of a ­Congruent Melting Compound Magnesium Strontium Diborate MgSrB2O5." Zeitschrift für anorganische und allgemeine Chemie 640, no. 8-9 (March 25, 2014): 1805–9. http://dx.doi.org/10.1002/zaac.201400043.

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41

Wang, Xuefei, Ying Wang, Bingbing Zhang, Fangfang Zhang, Zhihua Yang, and Shilie Pan. "CsB4O6F: A Congruent-Melting Deep-Ultraviolet Nonlinear Optical Material by Combining Superior Functional Units." Angewandte Chemie 129, no. 45 (October 4, 2017): 14307–11. http://dx.doi.org/10.1002/ange.201708231.

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42

Surovtsev, N. V., V. K. Malinovskii, A. M. Pugachev, and A. P. Shebanin. "The nature of low-frequency Raman scattering in congruent melting crystals of lithium niobate." Physics of the Solid State 45, no. 3 (March 2003): 534–41. http://dx.doi.org/10.1134/1.1562243.

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43

Uda, Satoshi, Xinming Huang, and Shinji Koh. "Transformation of the incongruent-melting state to the congruent-melting state via an external electric field for the growth of langasite." Journal of Crystal Growth 281, no. 2-4 (August 2005): 481–91. http://dx.doi.org/10.1016/j.jcrysgro.2005.04.072.

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44

Velazquez, Miguel Angel Nuñez, and Fernando Juárez Lopez. "Investigations into the Growth of GaN Nanowires by MOCVD Using Azidotrimethylsilane as Nitrogen Source." Advanced Materials Research 875-877 (February 2014): 1483–89. http://dx.doi.org/10.4028/www.scientific.net/amr.875-877.1483.

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Abstract:
Gallium trichloride (GaCl3) and azidotrimethylsilane (CH3)3SiN3were employed as alternatives gallium and nitrogen precursors respectively in the growth of GaN nanowires via a metal-organic chemical vapor deposition (MOCVD) system. Au pre-deposition on Si (100) substrate was using as catalysis seed to grown of GaN nanowires. X-Ray, FE-SEM and AFM analyses reveal that nanowires grown at temperature 1050 C present morphology characteristic to model VLS. Scanning electron microscopy reveal a surface morphology made up of wurzite that suggests that wires growth involve a melting process. A nucleation and growth mechanism, involving the congruent melting clusters of precursor molecules on the hot substrate surface, is therefore invoked to explain these observations. We attributed the improved growth behavior to the nearer-to-equilibrium growth and may be close to local thermodynamic equilibrium.
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45

UTSUMI, Wataru, Hiroyuki SAITOH, Katsutoshi AOKI, Hiroshi KANEKO, and Koji KIRIYAMA. "Congruent Melting of Gallium Nitride under High Pressure and Its Application to Single Crystal Growth." Nihon Kessho Gakkaishi 46, no. 4 (2004): 297–303. http://dx.doi.org/10.5940/jcrsj.46.297.

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46

Spivak, A. V., L. S. Dubrovinsky, and Yu A. Litvin. "Congruent melting of Ca-carbonate in static experiment at 3500 K and 10-22 GPa." Vestnik Otdelenia nauk o Zemle RAN 3, Special Issue (June 17, 2011): 1–7. http://dx.doi.org/10.2205/2011nz000220.

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47

Utsumi, Wataru, Hiroyuki Saitoh, Hiroshi Kaneko, Tetsu Watanuki, Katsutoshi Aoki, and Osamu Shimomura. "Congruent melting of gallium nitride at 6 GPa and its application to single-crystal growth." Nature Materials 2, no. 11 (October 26, 2003): 735–38. http://dx.doi.org/10.1038/nmat1003.

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48

Yu, Hongwei, Shilie Pan, Hongping Wu, Wenwu Zhao, Fangfang Zhang, Hongyi Li, and Zhihua Yang. "A new congruent-melting oxyborate, Pb4O(BO3)2with optimally aligned BO3triangles adopting layered-type arrangement." J. Mater. Chem. 22, no. 5 (2012): 2105–10. http://dx.doi.org/10.1039/c1jm14590h.

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49

Chaudhuri, S. P. "Melting/decomposition of mullite: incongruent or congruent? I. Phase equilibria of the system Al2O3SiO2." Ceramics International 13, no. 3 (January 1987): 167–75. http://dx.doi.org/10.1016/0272-8842(87)90027-7.

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50

Chaudhuri, S. P. "Melting/decomposition of mullite: incongruent or congruent? II. Responsible factors for dual nature of mullite." Ceramics International 13, no. 3 (January 1987): 177–81. http://dx.doi.org/10.1016/0272-8842(87)90028-9.

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