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Yıl 2018, Cilt: 22 Sayı: 5, 1221 - 1233, 01.10.2018
https://doi.org/10.16984/saufenbilder.344752

Öz


Kaynakça

  • [1] V.L. Ginzburg, E.A. Andryushin, Superconductivity, Revised ed. World Scientific Pub. Co. Inc., 2004.
  • [2] M. Hiroshi, T. Yoshiaki, F. Masao and A. Toshihisa, “A new high-Tc oxide superconductor without a rare earth element,” Japanese Journal of Applıed Physıcs Part 2-Letters, vol. 27, no. 2, pp. L209–L210, 1988.
  • [3] P. A. Lee and N. Read, “Why is Tc of the oxide superconductors so low,” Physical Review Letters, vol. 58, no. 25, pp. 2691–2694, 1987.
  • [4] K. Levin, J. H. Kim, J. P. Lu and Q. Si, “Normal state properties in the cuprates and their Fermi-liquid based interpretation,” Physica C, vol. 175, no. 5–6, pp. 449–522, 1991.
  • [5] G. Yildirim, M. Dogruer, F. Karaboga and C. Terzioglu, “Formation of nucleation centers for vortices in Bi-2223 superconducting core by dispersed Sn nanoparticles,” Journal of Alloys and Compounds, vol. 584, pp. 344–351, 2014.
  • [6] O. Gorur, C. Terzioglu, A. Varilci and M. Altunbas, “Investigation of some physical properties of silver diffusion-doped YBa2Cu3O7-x superconductors,” Superconductor Science & Technology, vol. 18, no. 9, pp. 1233–1237, 2005.
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Determination of Solubility Characteristic of (Bi, Gd) Substitution in Bi-2223 Inorganic Compounds

Yıl 2018, Cilt: 22 Sayı: 5, 1221 - 1233, 01.10.2018
https://doi.org/10.16984/saufenbilder.344752

Öz

In this study, it is examined the significant variations in the superconducting, electrical and structural
belongings of Bi-site Gd nanoparticle substituted Bi-2223 crystal. The Bi2.0-xGdxSr2.0Ca2.1Cu3.2Oy
(0≤x≤0.3) materials obtained with the standard solid state reaction technique are characterized by dc
resistivity (ρ-T), X-ray diffraction (XRD) and transport critical current density (Jc) measurements.
Moreover, all experimental findings as regards room temperature resistivity, residual resistivity, critical
transition temperatures (


),
crystallinity, lattice constant parameters, average crystallite
size, phase fraction and strength quality of interaction between superconducting grains in the Bi-2223
ceramics declare that the structural, electrical and superconducting characteristics degrade systematically
with the ascending of the Gd substitution level in the Bi-2223 samples. Furthermore, the major reason of
the reduction trend observed especially in the electrical and superconducting features is in relation with the
hole localization problem in the Cu-O2 layers. In this regard, grain boundary weak connections, dislocations
and defects in the matrix considerably ascend with the enhancement of Gd nanoparticle substitution level.
As seen from XRD measurements, it is clearly determined that there seems to be a decrement in the Bi2223
phase with the enhancement of Gd inclusions up to the substitution amount of x=0.1. After this critical
point, new characteristics peaks of Gd2O3 appear and measurement findings rapidly diminish to the
minimum values. This substitution level emphasizes that the solubility limit of Gd is noted to be x=0.1 for
Bi-2223. Likewise, the regular decrement observed c-axis length, critical current density and grain size
favors the regular retrogression of the superconducting characteristics.

Kaynakça

  • [1] V.L. Ginzburg, E.A. Andryushin, Superconductivity, Revised ed. World Scientific Pub. Co. Inc., 2004.
  • [2] M. Hiroshi, T. Yoshiaki, F. Masao and A. Toshihisa, “A new high-Tc oxide superconductor without a rare earth element,” Japanese Journal of Applıed Physıcs Part 2-Letters, vol. 27, no. 2, pp. L209–L210, 1988.
  • [3] P. A. Lee and N. Read, “Why is Tc of the oxide superconductors so low,” Physical Review Letters, vol. 58, no. 25, pp. 2691–2694, 1987.
  • [4] K. Levin, J. H. Kim, J. P. Lu and Q. Si, “Normal state properties in the cuprates and their Fermi-liquid based interpretation,” Physica C, vol. 175, no. 5–6, pp. 449–522, 1991.
  • [5] G. Yildirim, M. Dogruer, F. Karaboga and C. Terzioglu, “Formation of nucleation centers for vortices in Bi-2223 superconducting core by dispersed Sn nanoparticles,” Journal of Alloys and Compounds, vol. 584, pp. 344–351, 2014.
  • [6] O. Gorur, C. Terzioglu, A. Varilci and M. Altunbas, “Investigation of some physical properties of silver diffusion-doped YBa2Cu3O7-x superconductors,” Superconductor Science & Technology, vol. 18, no. 9, pp. 1233–1237, 2005.
  • [7] M. B. Turkoz, S. Nezir, C. Terzioglu, A. Varilci and G. Yildirim, “Investigation of Lu effect on YBa2Cu3O7-delta superconducting compounds,” Journal of Materials Science-Materials In Electronics, vol. 24, no. 3, pp. 896–905, 2013.
  • [8] Y. Zalaoglu, G. Yildirim, C. Terzioglu and O. Gorur, “Detailed analysis on electrical conduction transition from 2D variable range hopping to phonon-assisted 3D VRH mechanism belonging to Bi-site La substituted Bi-2212 system,” Journal of Alloys and Compounds, vol. 622, pp. 489–499, 2015.
  • [9] A. I. Abou-Aly, M. M. H. Abdel Gawad and R. Awad, “Improving the physical properties of (Bi, Pb)-2223 phase by SnO2 nano-particles addition,” Journal of Superconductivity and Novel Magnetism, vol. 24, no. 7, pp. 2077–2084, 2011.
  • [10] M. Takano, J. Takada, K. Oda, H. Kitaguchi, Y. Miura, Y. Ikeda, Y. Tomii and H. Mazaki, “High-Tc phase promoted and stabilized in the Bi, Pb-Sr-Ca-Cu-O system,” Japanese Journal of Applied Physics Part 2-Letters, vol. 27, no. 6, pp. L1041–L1043, 1988.
  • [11] C. Y. Shieh, Y. Huang, M. K. Wu and C. Y. Huang, “Preparation of single high-Tc phase Bi-Pb-Sr-Ca-Cu-O superconductor by the EDTA precursor solution method,” Physica C, vol. 185–189, pp. 513–514, 1991.
  • [12] S. A. Halim, A. K. Saleh, H. Azhan, S. B. Mohamed, K. Khalid and J. Suradi, “Synthesis of Bi1.5Pb0.5Sr2Ca2Cu3Oy via sol-gel method using different acetate-derived precursors,” Journal of Materials Science, vol. 35, no. 12, pp. 3043–3046, 2000.
  • [13] A. Tampieri, G. Celotti, S. Lesca, G. Bezzi, T. M. G. la Torretta and G. Magnani, “Bi(Pb)-Sr-Ca-Cu-O(2223) superconductor prepared by improved sol-gel technique,” Journal of the European Ceramic Society, vol. 20, no. 2, pp. 119–126, 2000.
  • [14] I. Hamadneh, A. Agil, A. K. Yahya and S. A. Halim, “Superconducting properties of bulk Bi1.6Pb0.4Sr2Ca2-xCdxCu3O10 system prepared via conventional solid state and coprecipitation methods,” Physica C, vol. 463–465, pp. 207–210, 2007.
  • [15] E. Yanmaz, I. H. Mutlu, S. Nezir and M. Altunbas, “Magnetic field dependence of samples of nominal composition Bi1.6Pb0.4Sr2Ca3Cu4Oy(2234) prepared by various techniques,” Journal of Alloys and Compounds, vol. 239, no. 2, pp. 142–146, 1996.
  • [16] H. B. Huang, G. F. de la Fuente, A. Sotelo, M. T. Ruiz, A. Larrea, L. A. Angurel and R. Navarro, “Ag/(Bi, Pb)-Sr-Ca-Cu-O superconducting tape processing-solid-state chemistry aspects,” Solid State Ionics, vol. 63–65, pp. 889–896, 1993.
  • [17] N. Ghanzanfari, A. Kılıç, A. Gencer and H. Ozkan, “Effects of Nb2O5 addition on superconducting properties of BSCCO,” Solid State Communications, vol. 144, no. 5–6, pp. 210–214, 2007.
  • [18] W. Zhu and P.S. Nicholson, “Atmosphere- temperature-time relationships for the formation of 110 K phase in the Bi-Pb-Sr-Ca-Cu-O superconductor system,” Applıed Physics Letters, vol. 61, no. 6, pp. 717–719, 1992.
  • [19] M. Borik, M. Chernikov, I. Dubov, V. Osiko, V. Veselago, Y. Yakowets and V. Stepankin, “Synthesis conditions superconduction properties of ceramic in the (Bi,Pb)-Sr-Ca-Cu-O system,” Superconductor Science & Technology, vol. 5, no. 3, pp. 151–155, 1992.
  • [20] R. Mawassi, S. Marhaba, M. Roumié, R. Awad, M. Korek and I. Hassan, “Improvement of Superconducting Parameters of Bi1.8Pb0.4Sr2Ca2Cu3O10+δ Added with Nano-Ag,” Journal of Superconductivity and Novel Magnetism, vol. 27, no. 5, 1131–1142, 2014.
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Toplam 65 adet kaynakça vardır.

Ayrıntılar

Birincil Dil İngilizce
Konular Malzeme Üretim Teknolojileri
Bölüm Araştırma Makalesi
Yazarlar

Yusuf Zalaoğlu

Yayımlanma Tarihi 1 Ekim 2018
Gönderilme Tarihi 17 Ekim 2017
Kabul Tarihi 12 Aralık 2017
Yayımlandığı Sayı Yıl 2018 Cilt: 22 Sayı: 5

Kaynak Göster

APA Zalaoğlu, Y. (2018). Determination of Solubility Characteristic of (Bi, Gd) Substitution in Bi-2223 Inorganic Compounds. Sakarya University Journal of Science, 22(5), 1221-1233. https://doi.org/10.16984/saufenbilder.344752
AMA Zalaoğlu Y. Determination of Solubility Characteristic of (Bi, Gd) Substitution in Bi-2223 Inorganic Compounds. SAUJS. Ekim 2018;22(5):1221-1233. doi:10.16984/saufenbilder.344752
Chicago Zalaoğlu, Yusuf. “Determination of Solubility Characteristic of (Bi, Gd) Substitution in Bi-2223 Inorganic Compounds”. Sakarya University Journal of Science 22, sy. 5 (Ekim 2018): 1221-33. https://doi.org/10.16984/saufenbilder.344752.
EndNote Zalaoğlu Y (01 Ekim 2018) Determination of Solubility Characteristic of (Bi, Gd) Substitution in Bi-2223 Inorganic Compounds. Sakarya University Journal of Science 22 5 1221–1233.
IEEE Y. Zalaoğlu, “Determination of Solubility Characteristic of (Bi, Gd) Substitution in Bi-2223 Inorganic Compounds”, SAUJS, c. 22, sy. 5, ss. 1221–1233, 2018, doi: 10.16984/saufenbilder.344752.
ISNAD Zalaoğlu, Yusuf. “Determination of Solubility Characteristic of (Bi, Gd) Substitution in Bi-2223 Inorganic Compounds”. Sakarya University Journal of Science 22/5 (Ekim 2018), 1221-1233. https://doi.org/10.16984/saufenbilder.344752.
JAMA Zalaoğlu Y. Determination of Solubility Characteristic of (Bi, Gd) Substitution in Bi-2223 Inorganic Compounds. SAUJS. 2018;22:1221–1233.
MLA Zalaoğlu, Yusuf. “Determination of Solubility Characteristic of (Bi, Gd) Substitution in Bi-2223 Inorganic Compounds”. Sakarya University Journal of Science, c. 22, sy. 5, 2018, ss. 1221-33, doi:10.16984/saufenbilder.344752.
Vancouver Zalaoğlu Y. Determination of Solubility Characteristic of (Bi, Gd) Substitution in Bi-2223 Inorganic Compounds. SAUJS. 2018;22(5):1221-33.

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