TY - JOUR
T1 - High-pressure synthesized nanostructural MgB2 materials with high performance of superconductivity, suitable for fault current limitation and other applications
AU - Prikhna, Tatiana A.
AU - Gawalek, Wolfgang
AU - Goldacker, Wilfried
AU - Savchuk, Yaroslav M.
AU - Noudem, Jacques
AU - Soldatov, Alexander
AU - Eisterer, Mikhael
AU - Weber, Harald W.
AU - Sokolovsky, Vladimir
AU - Serga, Maxim
AU - Dub, Sergey N.
AU - Wendt, Michael
AU - You, Shujie
AU - Sergienko, Nina V.
AU - Moshchil, Viktor E.
AU - Tkach, Vasiliy N.
AU - Dellith, Jan
AU - Karau, Friedrich
AU - Tomsic, Mikhael
AU - Shmidt, Christa
AU - Fesenko, Igor P.
AU - Habisreuther, Tobias
AU - Litzkendorf, Doris
AU - Meerovich, Viktor
AU - Sverdun, Vladimir B.
N1 - Funding Information:
and sample composition on the superconducting performance, didn’t lead to a consistent picture so far, but different key mechanisms could be identified. It has been show the importance of material densification to its performance. Dispersed inclusions of higher magnesium borides which are present in all types of materials obtained and obviously affect pinning, can be revealed by Raman spectroscopy, but the creation of Raman spectra database is still in progress. The Raman spectrum of MgB phase has been identified. As the synthesis pressure increases the stoichiometry of higher borides shifted to the formation of phases with higher boron concentration and material’s density increase. A carbon admixture in initial boron had the expected effect on the critical fields and promoted their increase. However, admixture of hydrogen provoked the increase of material porosity. High pressure produced MgB bulk materials are suitable for FCL applications, providing high current densities and the favorable heat capturing as well as for high magnetic field creation due to high and . ACKNOWLEDGMENT The authors gratefully acknowledge the financial grants supported the BMBF, Germany-Ukrainian and Austrian-Ukrainian scientific and technological cooperation and the grant from the Swedish Institute (SI).
Funding Information:
Manuscript received August 06, 2010; accepted November 22, 2010. Date of publication January 06, 2011; date of current version May 27, 2011. This work was supported in part by the Projects STCU 3665, of Ukrainian-German Cooperation IB/BMBF UKR 06/004, Ukrainian-Austrian Cooperation OEAD UA 13/2009 (M12-2009), Ukrainian-French Cooperation “Dnipro” No1969856 XF (M15-2009), H.C. Starck GmbH, Germany.
PY - 2011/6/1
Y1 - 2011/6/1
N2 - A variety of samples made via different routes were investigated. Samples are nanostructured (average grain sizes are about 20 nm). The advantage of high-pressure (HP)-manufactured (2 GPa, 800-1050°C, 1 h) MgB2 bulk is the possibility to get almost theoretically dense (1-2% porosity) material with very high critical current densities reaching at 20 K, in 0-1 T jc = 1.2 - 1.0 . 106 A/cm2(with 10% SiC doping) and jc = 9.2 - 7.3 105 A/cm2 (without doping). Mechanical properties are also very high: fracture toughness up to 4.4 ± MPa . m0.5 and 7.6 ± 2.0 MPa . m0.5 at 148.8 N load for MgB2 undoped and doped with 10% Ta, respectively. The HP-synthesized material at moderate temperature (2 GPa, 600°C, 1 h) fromB with high amount of impurityC(3.15%) andH(0.87%) has jc = 10 3 A/cm2 in 8 T field at 20 K, highest irreversibility fields (at 18.4 K Hirr = 15 T) and upper critical fields (at 22 K Hc2 = 15 T) but 17% porosity. HP materials with stoichiometry near MgB12 can have Tc = 37 K and jc = 6 . 10 4 A/cm2 at 0 T and Hirr = 5 T at 20 K. The spark plasma synthesized (SPS) material (50 MPa, 600-1050°C 1.3 h, without additions), demonstrated at 20 K, in 0-1 T jc = 4.5 - 4 10 5 A/cm2. Dispersed inclusions of higher magnesium borides, which are usually present in MgB2 structure and obviously create new pinning centers can be revealed by Raman spectroscopy (for the first time a spectrum of MgB was obtained). Tests of quench behavior, losses on MgB 7 rings and material thermal conductivity show promising properties for fault current limiters. Due to high critical fields, the material can be used for magnets.
AB - A variety of samples made via different routes were investigated. Samples are nanostructured (average grain sizes are about 20 nm). The advantage of high-pressure (HP)-manufactured (2 GPa, 800-1050°C, 1 h) MgB2 bulk is the possibility to get almost theoretically dense (1-2% porosity) material with very high critical current densities reaching at 20 K, in 0-1 T jc = 1.2 - 1.0 . 106 A/cm2(with 10% SiC doping) and jc = 9.2 - 7.3 105 A/cm2 (without doping). Mechanical properties are also very high: fracture toughness up to 4.4 ± MPa . m0.5 and 7.6 ± 2.0 MPa . m0.5 at 148.8 N load for MgB2 undoped and doped with 10% Ta, respectively. The HP-synthesized material at moderate temperature (2 GPa, 600°C, 1 h) fromB with high amount of impurityC(3.15%) andH(0.87%) has jc = 10 3 A/cm2 in 8 T field at 20 K, highest irreversibility fields (at 18.4 K Hirr = 15 T) and upper critical fields (at 22 K Hc2 = 15 T) but 17% porosity. HP materials with stoichiometry near MgB12 can have Tc = 37 K and jc = 6 . 10 4 A/cm2 at 0 T and Hirr = 5 T at 20 K. The spark plasma synthesized (SPS) material (50 MPa, 600-1050°C 1.3 h, without additions), demonstrated at 20 K, in 0-1 T jc = 4.5 - 4 10 5 A/cm2. Dispersed inclusions of higher magnesium borides, which are usually present in MgB2 structure and obviously create new pinning centers can be revealed by Raman spectroscopy (for the first time a spectrum of MgB was obtained). Tests of quench behavior, losses on MgB 7 rings and material thermal conductivity show promising properties for fault current limiters. Due to high critical fields, the material can be used for magnets.
KW - Boron compounds
KW - FCL behavior
KW - Magnetic variable measurement
KW - Pressure effects
KW - Raman spectroscopy
KW - Superconducting material growth
UR - http://www.scopus.com/inward/record.url?scp=79957965073&partnerID=8YFLogxK
U2 - 10.1109/TASC.2010.2096494
DO - 10.1109/TASC.2010.2096494
M3 - Article
AN - SCOPUS:79957965073
SN - 1051-8223
VL - 21
SP - 2694
EP - 2697
JO - IEEE Transactions on Applied Superconductivity
JF - IEEE Transactions on Applied Superconductivity
IS - 3 PART 3
M1 - 5680961
ER -