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1

Albutt, Naphat, Suejit Pechprasarn, Pattaraporn Damkoengsuntorn, and Thanapong Sareein. "The Giant Dielectric Constant of Y2NiMnO6 Ceramics for DC Bias." Applied Mechanics and Materials 866 (June 2017): 277–81. http://dx.doi.org/10.4028/www.scientific.net/amm.866.277.

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In this work, the uses of giant dielectric constant of Y2NiMnO6 ceramics were investigated in the frequency range from 1 kHz to 3 MHz. The Y2NiMnO6 ceramics were sintered at 1400 °C for 6, 12, 18 and 24 hours, respectively. The dielectric properties of Y2NiMnO6 ceramics were examined in dc bias from 0 to 1.5 volt at room temperature. We found that all sintering times displayed high dielectric permittivity at frequencies below 105 Hz, above which the values decreased significantly, applied dc bias also reduced dielectric permittivity. The peak of dielectric loss decreased significantly at high dc bias due to decreased contribution of dc conductivity in grain ceramics. This research has characterised electrical properties of Y2NiMnO6 ceramics which maybe suitable for electronic components including batteries and capacitors.
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2

Albutt, Naphat, Suejit Pechprasarn, Rukchanok Wanasuk, and Thanapong Sareein. "Electrical Impedance Properties of Y2NiMnO6 Ceramics for DC Bias at Atmosphere." Applied Mechanics and Materials 866 (June 2017): 251–55. http://dx.doi.org/10.4028/www.scientific.net/amm.866.251.

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The electrical impedance of Y2NiMnO6 ceramics sintered at 1400 °C for 6 to 24 hours were investigated. The electrical properties of Y2NiMnO6 ceramics were examined in dc bias from 0 volt to 1.5 volt at room temperature. At frequencies below 105 Hz the high electric impedance decreased significantly with longer sintering time, indicating that the grain and grain boundary effects. Increasing dc bias also reduced impedance at the lower frequencies, with polarisation affect at higher frequencies. This behaviour suggests a decrease in the relaxation time of the mobile charge carriers with increasing dc bias and describes a thermally activated relaxation phenomena in the Y2NiMnO6 ceramics.
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3

Sareein, Thanapong, Panakamon Deeyai, Bundit Putasaeng, and Naphat Chathirat. "Electrical Properties of Y2NiMnO6 Ceramics Sintered at High Temperature." Applied Mechanics and Materials 804 (October 2015): 55–58. http://dx.doi.org/10.4028/www.scientific.net/amm.804.55.

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In this work, impedance spectroscopy technique was used in order to investigate the electric properties of double perovskites of the Y2NiMnO6 ceramics, which were prepared by thermal decomposition technique at 800°C for 6 hours and then sintered at a high temperature of 1400°C for 6, 12, 18, and 24 hours. Consequently, the electric characterization of the Y2NiMnO6 ceramics was performed at 30°C °C in the frequency range from 102 Hz to 108 Hz. The results in the Rg with 10,000, 9,990, 6,400, and 1,700 (Ω) at sintering time, respectively. Dispersion was observed in the variation of impedance values with frequency. Possible reason for all the above observation was discussed.
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4

Su, J., Z. Z. Yang, X. M. Lu, J. T. Zhang, L. Gu, C. J. Lu, Q. C. Li, J. M. Liu, and J. S. Zhu. "Magnetism-Driven Ferroelectricity in Double Perovskite Y2NiMnO6." ACS Applied Materials & Interfaces 7, no. 24 (June 9, 2015): 13260–65. http://dx.doi.org/10.1021/acsami.5b00911.

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5

Zhang, Chenyang, Tingsong Zhang, Lei Ge, Shan Wang, Hongming Yuan, and Shouhua Feng. "Hydrothermal synthesis and multiferroic properties of Y2NiMnO6." RSC Adv. 4, no. 92 (October 3, 2014): 50969–74. http://dx.doi.org/10.1039/c4ra07099b.

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6

Deeyai, Panakamon, Thanapong Sareein, Bundit Putasaeng, and Naphat Chathirat. "Study Behavior of XPS Spectra of Ni, Mn, Y and O in Y2NiMnO6 Ceramics." Applied Mechanics and Materials 804 (October 2015): 97–103. http://dx.doi.org/10.4028/www.scientific.net/amm.804.97.

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Bulk Y2NiMnO6 samples were prepared by thermal decomposition technique at 800 °C for 6 hours. The effects of temperature on the structure of ceramics were investigated for different sintering temperatures in the range of 1000-1300 °C, while kept constant the sintering time of 12 hours. Structural characterization had been investigated via X-ray diffraction (XRD) on samples of different sintering temperatures. Results from the experiment had revealed that high temperature affected oxide in ceramic materials. Further analysis with X-ray photoelectron spectroscopy (XPS) technique had revealed an outstanding point of ceramics by investigating the Ni 2p, 2p3/2, Mn 2p1/2, 2p3/2, and Y 3d3/2, 3d5/2 at the surface of Y2NiMnO6 ceramics. The changes in relative intensity of XPS peaks and the shifts in their binding energy (eV) were observed in the results, while the effect of temperature on oxide in ceramics may be investigated with dielectric property in the future.
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7

Alam, Mahebub, Keshab Karmakar, Monalisa Pal, and Kalyan Mandal. "Electrochemical supercapacitor based on double perovskite Y2NiMnO6 nanowires." RSC Advances 6, no. 115 (2016): 114722–26. http://dx.doi.org/10.1039/c6ra23318j.

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The present work unveils the electrochemical properties of a newly emerging multiferroic material, double perovskite Y2NiMnO6, as an active material for the positive electrode of electrochemical supercapacitors.
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8

Kaippamagalath, Aswathi, Jasnamol P. Palakkal, Ajeesh P. Paulose, and Manoj R. Varma. "Structural and magnetic properties of multiferroic Y2NiMnO6 double perovskite." Ferroelectrics 518, no. 1 (October 3, 2017): 223–31. http://dx.doi.org/10.1080/00150193.2017.1360679.

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9

Alam, Mahebub, Kalyan Mandal, and Gobinda Gopal Khan. "Double perovskite Y2NiMnO6 nanowires: high temperature ferromagnetic–ferroelectric multiferroic." RSC Advances 6, no. 67 (2016): 62545–49. http://dx.doi.org/10.1039/c6ra10861j.

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10

Zhang, Chenyang, Tingsong Zhang, Lei Ge, Shan Wang, Hongming Yuan, and Shouhua Feng. "ChemInform Abstract: Hydrothermal Synthesis and Multiferroic Properties of Y2NiMnO6." ChemInform 46, no. 7 (January 29, 2015): no. http://dx.doi.org/10.1002/chin.201507005.

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11

Sharma, G., T. S. Tripathi, J. Saha, and S. Patnaik. "Magnetic entropy change and critical exponents in double perovskite Y2NiMnO6." Journal of Magnetism and Magnetic Materials 368 (November 2014): 318–23. http://dx.doi.org/10.1016/j.jmmm.2014.05.035.

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12

Deeyai, Panakamon, Thanapong Sareein, Bundit Putasaeng, and Naphat Chathirat. "Dielectric Properties of Y2NiMnO6 Ceramics at Various Sintering Times and Temperatures." Applied Mechanics and Materials 804 (October 2015): 16–20. http://dx.doi.org/10.4028/www.scientific.net/amm.804.16.

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Dielectric properties of hydrothermally decomposed Y2NiMnO6 ceramics prepared under several sintering conditions were investigated at room temperature. As the results, dielectric constants at 200 Hz were found about 928 and 23x103 for samples sintered at 1000 and 1400 oC, respectively. The dielectric permittivity for samples sintered at 1400 oC for different sintering times from 6 to 24 hours have yielded the best dielectric permittivity value of 104. On the other hand, low sintering temperature had resulted in smaller dielectric loss in comparison to larger dielectric loss generally found in the ceramics with high sintering temperature.
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13

Albutt, Naphat, Suejit Pechprasarn, Sangwoei Sawekwiharee, Anchana Kuttiyawong, Panakamon Thonglor, and Thanapong Sareein. "The Grain Structure of Nd Doped Y2NiMnO6 Ceramics Sintered at High Temperature." Applied Mechanics and Materials 879 (March 2018): 18–21. http://dx.doi.org/10.4028/www.scientific.net/amm.879.18.

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The granular structure of ceramic material influences the electrical properties. Ceramics of YMNO (Y2NiMnO6) doped with Nd were produced by compression and sintering. Grain size was determined from SEM image analysis. Generally, As the Nd dopant concentration was increased, the grain size increased with sintering time. However, at the highest dopant levels of 30% and 20% Nd, a large range in grain size was observed with regions of defective growth. In contrast, a more uniform grain growth was seen for the 10% Nd doped ceramic at all sintering times.
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14

Alam, Mahebub, and Kalyan Mandal. "Room temperature ferromagnetism and ferroelectricity in double perovskite Y2NiMnO6 thin film." Journal of Magnetism and Magnetic Materials 512 (October 2020): 167062. http://dx.doi.org/10.1016/j.jmmm.2020.167062.

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15

Xin, Chao, Bingqian Song, Zhixin Sun, Zhongxiang Hu, Boshi Yuan, Hui Li, Guangyong Jin, and Feng Pan. "Intrinsic role of ↑↑↓↓-type magnetic structure on magnetoelectric coupling in Y2NiMnO6." Applied Physics Letters 116, no. 24 (June 15, 2020): 242901. http://dx.doi.org/10.1063/5.0009568.

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16

Macedo Filho, Raimundo Bezerra, Alejandro Pedro Ayala, and Carlos William de Araujo Paschoal. "Spin-phonon coupling in Y2NiMnO6 double perovskite probed by Raman spectroscopy." Applied Physics Letters 102, no. 19 (May 13, 2013): 192902. http://dx.doi.org/10.1063/1.4804988.

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17

Tang, M. H., Y. G. Xiao, B. Jiang, J. W. Hou, J. C. Li, and J. He. "The giant dielectric tunability effect in bulk Y2NiMnO6 around room temperature." Applied Physics A 105, no. 3 (October 11, 2011): 679–83. http://dx.doi.org/10.1007/s00339-011-6608-5.

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18

Sareein, Thanapong, Panakamon Deeyai, Bundit Putasaeng, and Naphat Chathirat. "The Dielectric Property of Y2NiMnO6 Ceramics Sintered at High Temperature." Applied Mechanics and Materials 804 (October 2015): 108–12. http://dx.doi.org/10.4028/www.scientific.net/amm.804.108.

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The high dielectric permittivity of Y2NiMnO6 ceramics were measured by Agilent E4294A (Impedance Measurement) range of frequency 100 to 10 MHz in this research. In this sample ceramics, passing by a sintering temperature of 1400°C at 6 hours to 24 hours. The phase and microstructure of the deposited materials were investigated as a function of sintering temperature, using X-ray diffraction (XRD) and scanning electron microscopy (SEM). We found that the dielectric properties are very sensitive to the several sintered follow by time, and high temperature can be related to the change ordering of Ni2+ and Mn4+ ions.
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19

Albutt, Naphat, Suejit Pechprasarn, Sangwoei Sawekwiharee, Anchana Kuttiyawong, Panakamon Thonglor, and Thanapong Sareein. "Complete Phase Change of Y2NiMnO6 Ceramics Doped with TiO2 at High Temperature." Applied Mechanics and Materials 879 (March 2018): 47–50. http://dx.doi.org/10.4028/www.scientific.net/amm.879.47.

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Determining the structure of ceramic materials is essential in order to fully characterize the electrical properties and improve existing materials. YMNO ceramics (Y2NiMnO6) prepared by compression and sintering were doped with TiO2 and analyzed using XRD and SEM. The calcined sample prior to sintering contained phases of the YMNO double perovskite and TiO2. Following sintering at 1400°C, the perovskite structure was replaced by Y2Ti2O7 fcc structure, and the grain size was found to increase with sintering time up to 18 hours. This sets a limit to the amount of TiO2 which can be used to successfully dope the YMNO ceramic.
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20

Xie, Changzheng, and Lei Shi. "Tuning of magnetic properties for epitaxial Y2NiMnO6 thin film: Substrate is crucial." Applied Surface Science 384 (October 2016): 459–65. http://dx.doi.org/10.1016/j.apsusc.2016.05.046.

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21

Maiti, R. P., S. Dutta, M. Mukherjee, M. K. Mitra, and Dipankar Chakravorty. "Magnetic and dielectric properties of sol-gel derived nanoparticles of double perovskite Y2NiMnO6." Journal of Applied Physics 112, no. 4 (August 15, 2012): 044311. http://dx.doi.org/10.1063/1.4748058.

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22

Lei, Ming, Zhuo He, Zhijie Feng, and Yebin Xu. "Effects of PVA content on the synthesis of Y2NiMnO6 by sol–gel method." Journal of Sol-Gel Science and Technology 76, no. 1 (June 20, 2015): 204–9. http://dx.doi.org/10.1007/s10971-015-3767-4.

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23

Albutt, Naphat, Suejit Pechprasarn, Phimonkhae Chobdee, and Thanapong Sareein. "Studies of Dielectric Permittivity of Y2NiMnO6 Ceramics for DC Bias at Various Temperatures." Applied Mechanics and Materials 866 (June 2017): 272–76. http://dx.doi.org/10.4028/www.scientific.net/amm.866.272.

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The dielectric permittivity (ε) of Y2NiMnO6 ceramics prepared by sintering at 1400 °C over 6 to 24 hours was investigated. The response of the ceramics was measured from 1 kHz to 3 MHz, with the influence of a fixed dc bias from 0 to 1.5 V and temperature from 40 °C to -60 oC. Increasing dc bias was found to reduce ε' at low frequencies, while at higher frequencies the dc bias had less influence on ε'. At 40 °C a sharp transition from high to low ε' occurred starting at ~100 kHz, as the temperature of the ceramic was lowered, the transition shifted to lower frequencies. This behaviour is attributed to the charge ordering of Ni2+ and Mn4+ ions and the thermal effect on the ions energy.
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24

Cheng, Renfei, Zhijun Xu, Ruiqing Chu, Jigong Hao, Juan Du, and Guorong Li. "Microstructure and electrical properties of Bi1/2Na1/2TiO3–BaTiO3–Y2NiMnO6 lead-free piezoelectric ceramics." Ceramics International 41, no. 5 (June 2015): 6424–31. http://dx.doi.org/10.1016/j.ceramint.2015.01.080.

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25

Albutt, Naphat, Suejit Pechprasarn, and Thanapong Sareein. "Influence of Currents and Electric Fields in YNMO Ceramics." Applied Mechanics and Materials 866 (June 2017): 256–58. http://dx.doi.org/10.4028/www.scientific.net/amm.866.256.

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Development of ceramic materials is critical for new and improved electronic applications. Herein, the J-E response of Y2NiMnO6 (YNMO) ceramics composited by a solid state reaction method was investigated. Sintering temperature and time were found to have significant influence on the ceramics electrical properties. In particular, higher temperatures and longer sintering times resulted in more favourable dielectric properties of the YNMO ceramics. A current of 40 mA/cm2 at 20,000 mV/cm was obtained by sintering at 1300 °C for 12 hours, whereas a current of 9 mA/cm2 at 4000 mV/cm can be achieved by sintering at 1400 °C for 24 hours. These results will be useful for identifying applications for YNMO ceramics. The electrical properties of the YNMO ceramics can be tuned for different electronic components such as dry batteries and capacitors.
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26

Siritanon, Theeranun, Naphat Chathirat, Chivalrat Masingboon, Teerapon Yamwong, and Santi Maensiri. "Synthesis, characterization, and dielectric properties of Y2NiMnO6 ceramics prepared by a simple thermal decomposition route." Journal of Materials Science: Materials in Electronics 25, no. 3 (January 22, 2014): 1361–68. http://dx.doi.org/10.1007/s10854-014-1735-3.

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27

Alam, Mahebub, Kalyan Mandal, and Gobinda Gopal Khan. "Origin and tuning of room temperature ferromagnetism and ferroelectricity in double perovskite Y2NiMnO6 nanostructured thin films." Journal of Alloys and Compounds 822 (May 2020): 153540. http://dx.doi.org/10.1016/j.jallcom.2019.153540.

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28

Shen, Lei, Zhi Meng, Wenyi Liu, Xueli Xu, Tao Sun, Yonglai Liu, Wang Zhu, et al. "Manipulating the structural and magnetic properties of double perovskite Y2NiMnO6 thin films by oxygen pressure and buffer layer." Journal of Magnetism and Magnetic Materials 519 (February 2021): 167427. http://dx.doi.org/10.1016/j.jmmm.2020.167427.

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29

Mishra, Shubhankar, Amritendu Roy, Aditi Sahoo, Biswarup Satpati, Anirban Roychowdhury, P. K. Mohanty, Chandan Kumar Ghosh, and Dipten Bhattacharya. "Room-temperature surface multiferroicity in Y2NiMnO6 nanorods." Physical Review B 105, no. 23 (June 22, 2022). http://dx.doi.org/10.1103/physrevb.105.235429.

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30

Sharmili, T., A. Joana Preethi, J. Vigneshwaran, Sujin P. Jose, and M. Ragam. "Investigation on Y2NiMnO6 nanostructures for energy storage applications." Applied Physics A 129, no. 1 (December 20, 2022). http://dx.doi.org/10.1007/s00339-022-06322-1.

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