Investigation into the superconducting threshold of Bi1.6Pb0.4Sr2Can−1CunO2n+4+δ, n = 2, 2.5, 4 perovskites synthesized by glassy precursor route with Thermal and Raman spectroscopic techniques
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Abstract
Bi1.6Pb0.4Sr2Can−1CunOx perovskites system with n = 2, 2.5, and 4 synthesized through glassy precursor route by melt quenching. It has been found that only one composition of the series (n = 4), exhibited superconducting transition. Analysis by energy dispersive X-ray showed an increase of elemental ratio of Bi in all compositions. Activation energies of crystallization of various compositions are evaluated using thermal analysis and it is found that the activation energy plays a critical role in superconducting transition of these compounds. Structural analysis of the perovskites by XRD revealed a strikingly similar structure for all the compositions irrespective of their superconducting nature, while Raman and SEM revealed slight traces of impurity modes in all the compositions. However the impurity observed thus are minima in the lone composition that exhibited superconducting transition. Here an effort has been made to investigate the reasons for the only one composition of the series exhibiting superconducting transition irrespective of their near uniformity in the structure. It has been found that the presence of residual glass, plumbates and poor inter-grain connectivity formed the detrimental factors that made the two compositions devoid of their superconducting transition.
Keywords
Melt quenching Avrami index Crystallization kinetics Activation energy PBSCCONotes
Acknowledgments
Sincerely thanks Dr. Vasanth G Sathe, Raman Spectroscopy lab, Dr. Rajeev Rawat, Magneto Transport and Calorimetry Lab, UGC-DAE, CSR Indore, Madhya Pradesh, India for their useful discussion and support for the characterization of the above samples. Also thanks the Scientists at Advanced Material Characterization Division VSCC, Trivandrum, Kerala, India for extending their help to carry out the preparation of the above samples.
Supplementary material
References
- 1.Bahamani A, Sellami M, Bettahar N. Synthesis of bismuth mixed oxide by thermal decomposition of a coprecipitate precursor. J Therm Anal Calorim. 2012;107:955.CrossRefGoogle Scholar
- 2.Arshad M, Qureshi AH, Masud K, Qazi NK. Production of BSCCO bulk high Tc superconductors by sol-gel method and their characterisation by FTIR and XRD techniques. J Therm Anal Calorim. 2007;89:595.CrossRefGoogle Scholar
- 3.Aksan MA, Yakinici MA, Balci Y. Synthesis and characterisation of glass–ceramic Bi2−xGaxSr2Cu3O10+y superconductors. Supercond Sci Technol. 2000;13:958.CrossRefGoogle Scholar
- 4.Balci Y. Crystallisation kinetics of glass ceramic superconductors and investigation of the electrical conductivity properties. Ph D Thesis. Firat university, Elazig, Turkey. 1997.Google Scholar
- 5.Sato R, Komatsu T, Kuken Y, Matusita K, Sawada K, Hiraoka M. Effect of Cu+/Cu2+ ratio on the thermal stability and crystallization in Bi2Sr2CaCu2Ox glass. J. Non Crystalline Solid. 1993;152:150.CrossRefGoogle Scholar
- 6.Aksan MA, Yakinici ME, Balci Y. Thermal analysis study of Bi2Sr2Ca2ErxO10+δ glass ceramic system. J Therm Anal Calorim. 2005;81:418.CrossRefGoogle Scholar
- 7.Nillson A. ‘BSCCO superconductors processed by glass ceramic route’-Dissertation. 2008;65.Google Scholar
- 8.Matusita K, Sakka S. Kinetic study of the crystallization of glass by differential scanning calorimetry. Phys. Chem. Glass. 1979;20:81.Google Scholar
- 9.Cima MJ, Jiang XP, Chow HM, Huggerly JC, Flemings MC, Drody HD, Laudise RA, Johnson DW. Influence of growth parameters on the microstructure of directionally solidified Bi2Sr2CaCu2Oy. J.Mater. Res. 1990;5:1834.CrossRefGoogle Scholar
- 10.Nilson A, Gruner W, Acker J, Wetzig K. Critical aspects on preparation of Bi-2223 glassy precursor by melt process. J. Non Crystalline Solids. 2008;354:845.Google Scholar
- 11.Cardona M, Genzei L, Liu R, Wittlin A, Mattausch Hj, Garcia-Alvarado, Garcia-Gonzalez E. Infrared and Raman spectra of the MgBa2Cu3O7-type high Tc superconductors. Solid State Commun. 1987;64:727.CrossRefGoogle Scholar
- 12.Cardona M, Thomsen C, Liu R, VonSchering HG, Hartweg M, Yan YF, ZN Zhao ZN. Raman scattering on superconducting crystals of Bi2(sr1−xCax)n+2Cun+1O(6+2n)+δ(n = 0,1). Solid State Commun. 1988;66(12):1225.CrossRefGoogle Scholar
- 13.Pantoja AE, Pooke DM, Trodahl HJ, Irwin JC. Oxygen effect on the high frequency Raman phonons on Bi2Sr2CaCu2O8+δ. Phys Rev. B. 1998;58:5219.CrossRefGoogle Scholar
- 14.Carvalho CL, Guedes I. Spectroscopic characterisation of BPSCCO thin films grown by dip coating technique. Phys C. 2003;390(3):242.CrossRefGoogle Scholar
- 15.Zhang LW, Wang ZY, Gong SM, Chen TG. Lead diffusion and segregation in Pb doped Bi-2223 Physica–C Superconductivity and its Applications. 1997; 283:1092.Google Scholar
- 16.Popovic ZV, Thomson C, Cardona M, Liu R, Stanisic G, Kremmer R, Koenig W. Phonon characterisation of Bi2(Sr1−xCax)2CuO6+δ by infrared and Raman spectroscopy. Solid State Commun. 1988;66(9):965.CrossRefGoogle Scholar
- 17.Kakihana M, Osada M, Kall M, Borjesson L, Mazaki H, Yasuoka H, Yashima M, Yoshimura M. Raman-active phonons in Bi2Sr2Ca1−xYxCu2O8+δ(x = 0 − 1): effects of hole filling and internal pressure induced by Y doping for Ca, and implications for phonon assignments. Phys. Rev. B. 1996;53:11796–11806.CrossRefGoogle Scholar
- 18.Bellini V, Manghi F, Thonhauser T, Ambrosch-Draxl C. Electron -electron correlation in Bi2Sr2CaCu2O8. Phys. Rev. B. 2004;69:184508.CrossRefGoogle Scholar