Effect of aromatic hydrocarbon addition on in situ powder-in-tube processed MgB 2

Similar documents
Fabrication of high performance MgB 2 wires by an internal Mg diffusion process

EFFECTS OF SINTERING TEMPERATURE ON SUPERCONDUCTIVITY IN Ti-SHEATHED MgB 2 WIRES. G. Liang 1, H. Fang 1, S. Guchhait 2, C. Hoyt 1, J. T.

Influence of Ball-Milled Low Purity Boron Powder on the Superconductivity of MgB2

High transport critical current density above 30 K in pure Fe-clad MgB 2 tape

Phase transformation and superconducting properties of MgB2 using ball-milled low purity boron

Effect of grain size and doping level of SiC on the superconductivity and critical current density in MgB/sub 2/ superconductor

THE COMBINED INFLUENCE OF SiC AND RARE-EARTH OXIDES DOPING ON SUPERCONDUCTING PROPERTIES OF MgB 2 WIRES

Improvement of the critical current of in situ Cu-sheathed MgB 2 wires by copper additions and toluene doping

Enhancement of J C -B Properties in MoSi 2 doped MgB 2 tapes

A cheap liquid additive from acetone for strong in-field J c enhancement in MgB 2 conductors

Fabrication and transport critical currents of multifilamentary MgB 2 /Fe wires and tapes

Benzoic acid doping to enhance electromagnetic properties of MgB2 superconductors

Effect on deformation process of adding a copper core to multifilament MgB2 superconducting wire

Carbon Doping of MgB 2 by Toluene and Malic-Acid-in-Toluene

Tube filling technique influence on superconductivity in MgB 2 -based conductors prepared using laboratory made boron

The doping effect of multiwall carbon nanotube on MgB2/Fe superconductor wire

High-energy ball milling and Synthesis temperature study to improve superconducting properties of MgB 2 ex-situ tapes and wires

Enhancement of the critical current density and flux pinning of MgB2 superconductor by nanoparticle SiC doping

Evolution of tetragonal phase in the FeSe wire fabricated by a novel

Synergetic combination of LIMD with CHPD for the production of economical and high performance MgB2 Wires

Development of Doped MgB 2 Wires and Tapes for Practical Applications

The doping effect of multiwall carbon nanotube on MgB 2 /Fe. superconductor wire

Superconducting and thermal properties of ex-situ GlidCop sheathed multifilamentary MgB 2 wires

Scientific council of Faculty of Electrical Engineering and Information Technology. Slovak University of Technology in Bratislava

Superconducting properties of the powder-in-tube Cu-Mg-B and Ag-Mg-B wires

Enhancement of connectivity and flux pinning in MgB2 superconducting bulks and wires

Hot isostatic pressing of powder in tube MgB 2 wires

Transport properties and microstructure of mono- and seven-core wires of FeSe 1-x Te x

Effect of the starting boron powder on the superconducting properties of MgB

Effect of sintering temperature on the superconducting properties of graphene doped MgB2

We have fabricated a series of ex situ copper sheathed powder-in-tube MgB 2 wires

Hot pressing to enhance the transport J c of Sr 0.6 K 0.4 Fe 2 As 2. superconducting tapes

Flux pinning and inhomogeneity in magnetic nanoparticle doped MgB2/Fe wires

Phase formation in Cu-sheathed MgB 2 wires

Recent progress in melt-processed (Nd Sm Gd)Ba 2 Cu 3 O y superconductors

Superconducting transition width under magnetic field in MgB2 polycrystalline samples

80 Development of REBa2Cu3Ox Coated Conductor on Textured Metal Substrate

Inducement of superconductivity in Fe(Te,S) by sulfuric acid treatment

The Effect of Dopant Additions on the Microstructure of Boron Fibers Before and After Reaction to MgB 2

University of Wollongong. Research Online

High critical current densities in superconducting MgB 2 thin films

FORMING OF FULLERENE-DISPERSED ALUMINUM COMPOSITE BY THE COMPRESSION SHEARING METHOD

Preamble. It represents the known binary compounds showing SC at the highest temperature to date. No weak links. Possibility to incresase J c and H c2

Effect of Irradiation on the Superconductor Properties of Bi 2 Sr 2-x Li x Ca 2 Cu 3 O y

Evidence of high intergrain critical current density in fine grain (Ba 0.6 K 0.4 )Fe 2 As 2 wires and bulks

Pinning enhancement in MgB 2 superconducting thin films by magnetic nanoparticles of Fe 2 O 3

Forschungszentrum Karlsruhe - Institut für Technische Physik (ITP), P.O. Box 3640, D Karlsruhe, Germany.

Weak links and phase slip centers in superconducting MgB 2 wires

Effect of synthesis temperature on superconducting properties of n-sic added bulk MgB 2 superconductor

Formation of High-Field Pinning Centers in Superconducting MgB 2 Wires by Using High Hot Isostatic Pressure Process

Effect of grain refinement on enhancing critical current density and

Mechanical Properties of Bulk Metallic Glasses and composites

PS-014 INFLUENCE OF SINTERING TIME ON THE PROPERTIES OF HIGH TEMPERATURE SUPERCONDUCTOR BPSCCO BASED. Eidi Sihombing

Strongly connected ex-situ MgB 2 polycrystalline bulks fabricated. by solid-state self-sintering

Composite. Department of Physics, Banaras Hindu University, Varanasi , India

A study of the sintering behaviour of magnesium diboride. Department of Materials, University of Oxford, Parks Road, Oxford, OX1 3PH, UK.

M gb 2 superconducting bulk magnet realizes highly homogeneous

MA-SHS of ZrC and ZrB2 in Air from The Zr/B/C Powder. the original is available online at Instructions for use

Preparation and Physical Properties of Tl 0.65 Hg 0.35 Ba 2 Ca n-1 Cu n O 2n+3 δ (n = 1, 2, 3) Superconductors

ISSN GANENDRA, Vol. V, No. 1. PREPARATION AND CHARACTERIZATION OF TRANSPARENT CONDUCTIVE ZnO THIN FILMS BY DC MAGNETRON SPUTTERING

The manufacturing of an electroplated Ni layer on texturedcusubstratefor Cu-based HTS coated conductors

STUDYING AMORPHOUS-CRYSTALLINE TRANSITIONS IN POWDERS CAUSED BY BALL-MILLING

Formation and Soft Magnetic Properties of Co Fe Si B Nb Bulk Glassy Alloys

Effect of SiC Whiskers on Properties of SiC Coating for. Carbon/carbon Composites

GIOVANNI GIUNCHI EDISON S.p.a. Divisione Ricercs e Sviluppo Via U. Bassi Milano (Italy)

University of Wollongong. Research Online

Direct Observation of nm-scale Mg- and B-Oxide Phases at Grain Boundaries in MgB 2

MICROSTRUCTURE AND MECHANICAL PROPERTIES OF POWDER ALUMINIUM PREPARED BY SEVERE PLASTIC DEFORMATION

ENHANCEMENT OF MECHANICAL PROPERTIES FOR SELF-REINFORCED HOT-PRESSED SILICON CARBIDE

Flux pinning force in bulk MgB 2 with variable grain size

SUPPLEMENTARY INFORMATION

SEM and TEM Characterization of Magnesium Hydride Catalyzed. with Ni Nano-Particle or Nb 2 O 5. and Hironobu Fujii a) Abstract

STRUCTURAL PROPERTIES AND COMPOSITION ANALYSIS OF Cu Ni Co ALLOY THIN FILM

Current Status of the KSTAR TF Superconducting Magnet Development

Microstructure and superconducting properties of hot isostatically pressed MgB 2. T C Shields, K Kawano, D Holdom and J S Abell

Synthesis of MgB 2 from magnesium rich powders

Microstructural Evolution of Ti-Mo-Ni-C Powder by Mechanical Alloying

Fabrication of Textured β-si 3 N 4 and β-sialon by Slip Casting in A Strong Magnetic Field and Reaction-Sintering

Superconducting Thick Films on Commercial Silver Substrates

Bonding strength of Al/Mg/Al alloy tri-metallic laminates fabricated

ON THE HALL EFFECT AND MAGNETORESISTANCE OF Co Fe 4.5 Si B 15 Mo 2 AMORPHOUS AND CRYSTALLIZED RIBBONS

Axial strain effects of superconducting properties in detwinned RE123 coated conductors.

Synthesis of Dense Bulk MgB2 by Infiltration and Growth

Development of Ultra-Carbon Steel Prepared by Mechanical Alloying and Subsequent Hot Pressing

Towards the Realization of Higher Connectivity in MgB 2 Conductors: In-situ or Sintered Ex-situ?

Effects of CaO B 2 O 3 Glass on Sintering and Microwave Properties of Cordierite Ceramics for Low-Temperature Cofired

New Cu-based Bulk Metallic Glasses with High Strength of 2000 MPa

Fabrication and characterization of superconducting PLD MgB2 thin films

Deposition of biaxially aligned YSZ layers by dual unbalanced magnetron sputtering.

Transport critical current, anisotropy, irreversibility fields and exponential

Y.S. Pyoun 1, 2, I.H. Cho 2, C.M. Suh 3, J. Park 4, J. Rogers 5, R. Kayumov 1 and R. Murakami 6

Demonstration of an iron-pnictide bulk superconducting magnet capable of trapping over 1 T

Soft Magnetic Properties of Nanocystalline Fe Si B Nb Cu Rod Alloys Obtained by Crystallization of Cast Amorphous Phase

Supplementary Figure 1: Photograph of our FeSe single crystals and the rocking curve of the co-aligned crystals. (a) Photograph of representative

Influence of thermochemical treatments on TSMG YBCO bulks doped with Li and Al

Doping Effect of Nano-Diamond on Superconductivity and Flux Pinning in MgB 2

Supporting Online Material for

ESTIMATION OF LUBRICITY BY NUMERICAL METHOD ON SURFACE OF NBC-REINFORCED TOOL FOR HOT STEEL ROLLING

Aluminum foil reinforced by carbon nanotubes

Sn wires with enhanced characteristics

Transcription:

Effect of aromatic hydrocarbon addition on in situ powder-in-tube processed MgB 2 tapes H. Yamada General Technology Division, Central Japan Railway Company, 1545-33, Ohyama, Komaki, Aichi 485-0801, Japan M. Hirakawa Construction Department, Central Japan Railway Company, 2-1-85, Kounan, Minato-ku, Tokyo 108-8204, Japan H. Kumakura and H. Kitaguchi Superconducting Materials Center, National Institute for Materials Science, 1-2-1, Sengen, Tsukuba, Ibaraki 305-0047, Japan We fabricated in situ powder-in-tube processed MgB 2 /Fe tapes using aromatic hydrocarbon of benzene, naphthalene, and thiophene as additives, and investigated the superconducting properties. We found that these aromatic hydrocarbons were very effective for increasing the Jc values. The Jc values of 20mol% benzene-added tapes reached 130A/mm 2 at 4.2K and 10T. This value was almost comparable to that of 10mol% SiC-added tapes and about four times higher than that of tapes with no additions. Microstructure analyses suggest that this Jc enhancement is due to both the substitution of carbon for boron in MgB 2 and the smaller MgB 2 grain size. The MgB 2 superconductor is expected to be applied to practical superconducting wires because its transition temperature, 39K, is much higher than those of conventional metallic superconductors. The lower cost of the raw materials, Mg and B, than that of Nb, is an additional advantage of MgB 2. Recently, small coils using MgB 2 wires have been produced. In order to evaluate the potential of MgB 2 for power applications, wire processing techniques are now being actively developed throughout the world. The most popular method is the so-called in situ powder-in-tube (PIT) method,

where constituent powder was packed into a metal tube and cold-worked into wires. 1-3 However, it is necessary to increase the upper critical field and the critical current density to develop useful MgB 2 superconducting wire. To improve these properties, various methods have been reported. They include, for example, the ball-milling method 4,5, the addition of nanometer-size SiC powder 6, the use of MgH 2 powder instead of Mg powder 7, and the use of nanometer-size Mg powder 8. The addition of nanometer-size SiC powder is effective to increase B c2 and, hence, Jc in high magnetic fields. This Jc improvement should be attributed to the substitution of carbon from SiC for boron in MgB 2. 9 In this letter, we used aromatic hydrocarbons of benzene (C 6 H 6 ), naphthalene (C 10 H 8 ), and thiophene (C 4 H 4 S) as additives and succeeded in significantly improving the superconducting properties of MgB 2 tapes. We fabricated C 6 H 6 -, C 10 H 8 -, and C 4 H 4 S-added MgB 2 tapes by the in situ PIT method. Commercial MgH 2 powder, commercial amorphous B powder, and 10-20mol% C 6 H 6, 10mol% C 10 H 8, or 10mol% C 4 H 4 S were mixed. In order to avoid the evaporation or sublimation of the added aromatic hydrocarbons, the powders were mixed for 1 hour using the ball-milling method. The milling was carried out by using a pot and balls made of tungsten-carbide under a high-purity argon gas atmosphere. The mixed powders were put into pure Fe tubes with 6mm in outer diameter and 3.5mm in inner diameter and cold-rolled into tapes with 4mm in width and 0.5mm in thickness using groove-rolling and flat-rolling machines. The mixing of powders and packing of the mixed powder into Fe tubes were carried out under a high-purity argon gas atmosphere by using a glove box in order to avoid the oxidation of the powders. Heat treatment was carried out at 600 o C for 1 hour under a flowing argon gas atmosphere. As a reference, 10mol% SiC-added MgB 2 tapes with the same size were also fabricated. The transport critical current, Ic, was measured by a standard four-probe resistive method at 4.2K in magnetic fields. Current and voltage leads were directly soldered to the Fe sheaths of the tapes. Ic measurements were carried out at 4.2K in magnetic fields below 12T. The field was applied parallel to the main plane of the tapes. The criterion of Ic definition was 1µV/cm. Figure 1 summarizes the field dependence of Jc at 4.2K for the C 6 H 6 -, C 10 H 8 -, and C 4 H 4 S-added tapes. As a reference, the data of the pure and 10mol% SiC-added tapes are also shown in the figure. The aromatic hydrocarbon-added tapes show much higher Jc than the pure tape. The

field dependence of Jc was also improved by the aromatic hydrogen additions, suggesting that B c2 was enhanced by the additions. The 20mol% C 6 H 6 -added tape shows the highest Jc of 130A/mm 2 at 4.2K and 10T among the aromatic hydrocarbon-added tapes. This Jc was about four times higher than that of pure tape and almost comparable to that of the 10mol% SiC-added tape. In magnetic fields lower than 8T, C 6 H 6 -added tapes show higher Jc than the 10mol% SiC-added tape. However, the field dependence of Jc for aromatic hydrocarbon-added tapes is slightly larger than that of the SiC-added tape. This can be explained by the difference in the carbon substitution level, as discussed later. The results in Fig. 1 suggest that another aromatic hydrocarbon addition is also effective to enhance the Jc-B properties of MgB 2 tapes. Figure 2 shows the X-ray diffraction (XRD) pattern of the 10mol% C 6 H 6 -added tape. This XRD pattern reveals that MgB 2 was obtained as the nearly single phase. We calculated the a-axis and c-axis lengths of the crystalline MgB 2 core from the (110) and (002) x-ray diffraction peaks, respectively. Figures 3(a) and (b) show the a- and c-axis lengths as a function of the additive content. As a reference, the a- and c-axis lengths of the tape prepared with the SiC powder addition are also included in the figure. It was reported that, for the SiC-added tape, the a-axis length shrank, while the c-axis did not change due to the substitution of the carbon from SiC powder for boron. 9 Similar changes of the a- and c-axis lengths were also observed for C 6 H 6 -, C 10 H 8 -, and C 4 H 4 S-added tapes, although the decrease of the a-axis length is almost independent of the amount of C 6 H 6. This result indicates that the substitution of carbon for boron also occurs in the aromatic hydrocarbon-added tapes. Figure 3(a) indicates that the a-axis length of the 10mol% C 6 H 6 -added tape was almost comparable to that of the tape prepared with the 2-3mol% SiC powder addition. M. Avdeev et al. summarized the a-axis of several MgB 2 samples as a function of carbon substitution, x, in Mg(B 1-x C x ) 2. 10 Based on these a-axis vs. x curves, the amounts of substituted carbon x in our samples were estimated to be ~0.015 and ~0.03 for the aromatic hydrocarbon-added tapes and 10mol% SiC-added tape, respectively. This smaller amount of carbon substitution for aromatic hydrocarbon additions is the reason that the field dependence of Jc for the aromatic hydrocarbon-added tapes is slightly larger than that of the 10mol% SiC-added tape, as shown in Fig. 1. This amount of substituted carbon for aromatic hydrocarbon-added tapes was much smaller than the 10-20mol% of aromatic hydrocarbon added to the starting powder. Thus, most of the added

aromatic hydrocarbons seemed to be vaporized from both ends of the tape during the heat treatment. Figure 4 shows a comparison of scanning electron micrographs of the fractured surfaces of the MgB 2 cores removed from the (a) pure and (b) 10mol% C 6 H 6 -added tapes. Both MgB 2 cores show a similar microstructure; however, the MgB 2 grain size of the tapes prepared with the C 6 H 6 addition is smaller than that of tapes with no additions. In conclusion, the addition of an aromatic hydrocarbon, such as C 6 H 6, C 10 H 8, and C 4 H 4 S to the starting powder mixture was effective to increase the Jc values of in situ-processed MgB 2 tapes. The Jc value of the tapes prepared with the 20mol% C 6 H 6 addition reached 130A/mm 2 at 4.2K and 10T. This Jc value was almost comparable to that of the tapes prepared with the 10mol% SiC powder addition and about four times higher than that of tapes with no additions. We consider that there are two factors for the Jc increase observed in the aromatic hydrocarbon-added tapes. (1) The carbon atoms of C 6 H 6, C 10 H 8, and C 4 H 4 S were substituted for boron, and this substitution enhanced B c2 and, hence, increased Jc at high fields. This effect is similar to the effect of the addition of nanometer-size SiC powder. (2) The MgB 2 grain size of the tapes prepared with the C 6 H 6 addition was smaller than that of tapes with no additions. Such a small MgB 2 grain size is effective to enhance flux pinning because the grain boundaries of MgB 2 represent effective pinning centers.

References 1. S. Jin, H. Mavoori, and R.B. van Dover, Nature 411, 563 (2001). 2. B.A. Glowacki, M. Majoros, M. Vickers, J.E. Evetts, Y. Shi, and I. McDougall, Supercond. Sci. Technol. 14, 93 (2001). 3. H. Suo, C. Beneduce, M. Dhalle, N. Musolino, J.-Y. Genoud, and R. Flukiger, Appl. Phys. Lett. 79, 3116 (2001). 4. H. Fang, S. Padmanabhan, Y.X. Zhou, and K. Salama, Appl. Phys. Lett. 82, 4113 (2003). 5. C. Fischer, C. Rodig, W. Hassler, O. Perner, J. Eckert, K. Nenkov, G. Fuchs, H. Wendrock, B. Holzapfel, and L. Schultz, Appl. Phys. Lett. 83, 1803 (2003). 6. S.X. Dou, S. Soltanian, J. Horvat, X.L. Wang, S.H. Zhou, M. Ionescu, H.K. Liu, P. Munroe, and M. Tomsic, Appl. Phys. Lett. 81, 3419 (2002). 7. H. Fujii, K. Togano, and H. Kumakura, Supercond. Sci. Technol. 15, 1571 (2002). 8. H. Yamada, M. Hirakawa, H. Kumakura, A. Matsumoto, and H. Kitaguchi, Appl. Phys. Lett. 84, 1728 (2004). 9. H. Kumakura, H. Kitaguchi, A. Matsumoto, and H. Yamada, Supercond. Sci. Technol. 18, 1042 (2005). 10. M. Avdeev, J.D. Jorgensen, R.A. Ribeiro, S.L. Bud ko, and P.C. Canfield, Physica C301, 387 (2003).

Fig. 1. Magnetic field dependence of Jc at 4.2K for the aromatic hydrocarbon-added MgB 2 /Fe tapes heat-treated at 600 o C for 1h. Fig. 2. X-ray diffraction pattern of the MgB 2 /Fe tape prepared with the 10mol% benzene addition. Fig. 3. (a) a-axis and (b) c-axis lengths of the MgB 2 cores in the aromatic hydrocarbon- and SiC-added MgB 2 /Fe tapes, respectively. The horizontal axis shows the amount of additives. Fig. 4. Scanning electron micrographs of the fractured surfaces of the MgB 2 core removed from the (a) pure and (b) 10mol% benzene -added tapes. 1000 MgH 2 +B+SiC10mol% Jc(A/mm 2 ) 100 10 MgH 2 +B +Naphthalene10mol% MgH 2 +B +Thiophene10mol% MgH 2 +B 5 6 7 8 9 10 11 12 13 B(T) MgH 2 +B +Benzene20mol% MgH 2 +B +Benzene10mol% Fig.1

Intensity(a.u.) 002 110 20 30 40 50 60 70 80 2q(deg.) Fig.2 a-axis(nm) 0.3095 0.3090 0.3085 0.3080 SiC addition Benzene addition Naphthalene addition Thiophene addition c-axis(nm) 0.3550 0.3545 0.3540 0.3535 0.3530 0.3525 SiC addition Benzene addition Naphthalene addition Thiophene addition 0.3075 0 5 10 15 20 amount of additives(%) 0.3520 0 5 10 15 20 amount of additives(%) (a) (b) Fig.3

1µm (a) MgH 2 +B 1µm (b) MgH 2 +B+10mol%Benzene Fig.4