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Dive into the research topics where P.M. Martin is active.

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Featured researches published by P.M. Martin.


Applied Physics Letters | 1996

High critical current density superconducting tapes by epitaxial deposition of YBa2Cu3Ox thick films on biaxially textured metals

Amit Goyal; David P. Norton; J. D. Budai; M. Paranthaman; Eliot D. Specht; D. M. Kroeger; D. K. Christen; Qing He; B. Saffian; F.A. List; D.F. Lee; P.M. Martin; C.E. Klabunde; E. Hartfield; V.K. Sikka

A method to obtain long lengths of flexible, biaxially oriented substrates with smooth, chemically compatible surfaces for epitaxial growth of high‐temperature superconductors is reported. The technique uses well established, industrially scalable, thermomechanical processes to impart a strong biaxial texture to a base metal. This is followed by vapor deposition of epitaxial buffer layers (metal and/or ceramic) to yield chemically compatible surfaces. Epitaxial YBa2Cu3Ox films grown on such substrates have critical current densities exceeding 105 A/cm2 at 77 K in zero field and have field dependencies similar to epitaxial films on single crystal ceramic substrates. Deposited conductors made using this technique offer a potential route for the fabrication of long lengths of high‐Jc wire capable of carrying high currents in high magnetic fields and at elevated temperatures.


Science | 2006

High-Performance High-Tc Superconducting Wires

Sukill Kang; Amit Goyal; Jing Li; A.A. Gapud; P.M. Martin; L. Heatherly; James R. Thompson; D. K. Christen; F.A. List; M. Paranthaman; D.F. Lee

We demonstrated short segments of a superconducting wire that meets or exceeds performance requirements for many large-scale applications of high-temperature superconducting materials, especially those requiring a high supercurrent and/or a high engineering critical current density in applied magnetic fields. The performance requirements for these varied applications were met in 3-micrometer-thick YBa2Cu3O7-δ films epitaxially grown via pulsed laser ablation on rolling assisted biaxially textured substrates. Enhancements of the critical current in self-field as well as excellent retention of this current in high applied magnetic fields were achieved in the thick films via incorporation of a periodic array of extended columnar defects, composed of self-aligned nanodots of nonsuperconducting material extending through the entire thickness of the film. These columnar defects are highly effective in pinning the superconducting vortices or flux lines, thereby resulting in the substantially enhanced performance of this wire.


Journal of Applied Physics | 1995

Thermoelectric properties of CoSb3 and related alloys

J. W. Sharp; E.C. Jones; R. K. Williams; P.M. Martin; Brian C. Sales

Seebeck, electrical, and thermal conductivity data are reported on CoSb3, and doped and undoped alloys of Co1−x Ir x Sb3−y As y from 20 to 700 K. n‐type semiconductors were obtained by doping with Ni, Te, or Pd, and the hole concentration in p‐type samples was increased by substitution of Fe, Ru, Os, and Ge. An estimated maximum value for ZT of 0.6 (Z is the figure of merit) was found for a Te‐doped (n‐type) alloy at 700 K. For p‐type alloys, the maximum value of ZT was found to be 0.3 at 550 K. Electrical and thermal transport data also are reported for CoAs3, RhSb3, and IrSb3. Most of the samples investigated were polycrystalline, but a few measurements on CoSb3 single crystals also are discussed.


Journal of Applied Physics | 1995

Thermoelectric properties of CoSb{sub 3} and related alloys

J. W. Sharp; E.C. Jones; R. K. Williams; P.M. Martin; Brian C. Sales

Seebeck, electrical, and thermal conductivity data are reported on CoSb3, and doped and undoped alloys of Co1−x Ir x Sb3−y As y from 20 to 700 K. n‐type semiconductors were obtained by doping with Ni, Te, or Pd, and the hole concentration in p‐type samples was increased by substitution of Fe, Ru, Os, and Ge. An estimated maximum value for ZT of 0.6 (Z is the figure of merit) was found for a Te‐doped (n‐type) alloy at 700 K. For p‐type alloys, the maximum value of ZT was found to be 0.3 at 550 K. Electrical and thermal transport data also are reported for CoAs3, RhSb3, and IrSb3. Most of the samples investigated were polycrystalline, but a few measurements on CoSb3 single crystals also are discussed.


Physica C-superconductivity and Its Applications | 1997

Growth of biaxially textured buffer layers on rolled-Ni substrates by electron beam evaporation

M. Paranthaman; Amit Goyal; F.A. List; Eliot D. Specht; D.F. Lee; P.M. Martin; Qing He; D. K. Christen; David P. Norton; J. D. Budai; D. M. Kroeger

Abstract This paper describes the development of two buffer layer architectures on rolled-Ni substrates using an electron beam evaporation technique. The first buffer layer architecture consists of an epitaxial laminate of CeO 2 /Pd/Ni. The second alternative buffer layer consistes of an epitaxial laminate of YSZ/CeO 2 /Ni. The cube (100) texture in the Ni was produced by cold-rolling followed by recrystallization. The CeO 2 films were grown epitaxially on both Pd-buffered and textured-Ni substrates. The YSZ films were grown epitaxially on CeO 2 -buffered Ni substrates. The crystallographic orientation of the Pd, CeO 2 , and YSZ films were all (100). We also studied the effect of CeO 2 layer thickness and crack formation on textured-Ni substrates. The layer thickness was found to be critical. For some thickness, cracks formed in the CeO 2 layer. The presence of YSZ layers on the CeO 2 layers seem alleviate the cracks that are formed underneath. Our SEM studies showed that both CeO 2 (3–10 nm thick underlayer) and YSZ layers were smooth and continuous.


Physica C-superconductivity and Its Applications | 2001

Recent progress in the fabrication of high-Jc tapes by epitaxial deposition of YBCO on RABiTS

Amit Goyal; D.F. Lee; F.A. List; Eliot D. Specht; R. Feenstra; M. Paranthaman; X. Cui; S.W. Lu; P.M. Martin; D. M. Kroeger; D. K. Christen; B. W. Kang; David P. Norton; C. Park; D.T. Verebelyi; J. R. Thompson; R. K. Williams; Tolga Aytug; Claudia Cantoni

Abstract Progress made in the fabrication of rolling assisted biaxially textured substrates (RABiTS) and epitaxial deposition or formation of HTS on such substrates is reported. Significant progress has been made in understanding the role of meso-scale defects such as grain boundaries on long-range current flow of HTS conductors made using the RABiTS approach. Both experimental and theoretical calculations suggest that in well-textured samples these commonly present defects do not provide an intrinsic barrier to current flow in long-length conductors. Significant progress has also been made in the reel-to-reel deposition of oxide buffer layers and in the fabrication of long-length superconductors using the ex situ BaF 2 technique. Finally, non-magnetic, mechanically strengthened, biaxially textured metal templates have been fabricated with high quality oxide buffer layers. Epitaxial formation of YBCO on such substrates yields critical current densities over 1 MA/cm 2 at 77 K, 0 T.


Superconductor Science and Technology | 1999

Growth of biaxially textured RE2O3 buffer layers on rolled-Ni substrates using reactive evaporation for HTS-coated conductors

M. Paranthaman; D.F. Lee; Amit Goyal; Eliot D. Specht; P.M. Martin; X. Cui; John E. Mathis; R. Feenstra; D. K. Christen; D. M. Kroeger

In an effort to develop alternative single buffer layer architectures for YBCO (YBa2Cu3O7-y) coated conductors, we have studied RE2O3 (RE = Y, and rare earths) as candidate materials. High-quality Y2O3, Gd2O3 and Yb2O3 buffer layers were grown epitaxially on biaxially textured Ni (100) substrates using reactive electron beam evaporation. Using thermodynamic considerations for the formation of metal oxides, we employed both reducing atmospheres and water vapour to oxidize the film in situ to form stoichiometric RE2O3. We have also prevented NiO formation at the substrate-film interface during this process. Detailed x-ray studies have shown that the Y2O3, Gd2O3 and Yb2O3 films were grown with a single epitaxial orientation. The lattice mismatch between YBCO and Gd2O3 was small as compared with that of YBCO with other rare earth oxides. SEM micrographs indicated that ~0.5 ?m thick Y2O3 films on rolled-Ni substrates were dense, continuous and crack free. A high Jc of 1.8 ? 106 A cm-2 at 77 K and self-field was obtained on YBCO films grown on alternative buffer layers with a layer sequence of YBCO/Yb2O3 (sputtered)/Y2O3 (e-beam)/Ni.


Superconductor Science and Technology | 2003

Uniform performance of continuously processed MOD-YBCO-coated conductors using a textured Ni?W substrate

D.T. Verebelyi; U. Schoop; C. Thieme; Xiaoping Li; W. Zhang; T. Kodenkandath; Alexis P. Malozemoff; N. Nguyen; E. Siegal; David M. Buczek; Joseph Lynch; J. Scudiere; M.W. Rupich; Amit Goyal; Eliot D. Specht; P.M. Martin; M. Paranthaman

Second-generation coated conductor composite HTS wires have been fabricated using a continuous reel-to-reel process with deformation-textured Ni–W substrates and a metal-organic deposition process for YBa2Cu3O7−x. Earlier results on 1 m long and 1 cm wide wires with 77 K critical current performance greater than 100 A cm−1 width have now been extended to 7.5 m in length and even higher performance, with one wire at 132 and another at 127 A cm−1 width. Performance as a function of wire length is remarkably uniform, with only 2–4% standard deviation when measured on a 50 cm length scale. The length-scale dependence of the deviation is compared with a statistical calculation.


Journal of Materials Research | 2002

Comparative Study of Thickness Dependence of Critical Current Density of Yba 2 Cu 3 O 7–δ on (100) SrTiO 3 and on Rolling-assisted Biaxially Textured Substrates

B. W. Kang; A. Goyal; D.F. Lee; John E. Mathis; Eliot D. Specht; P.M. Martin; D. M. Kroeger; M. Paranthaman; S. Sathyamurthy

We investigated the dependence of critical current density ( J c ) on thickness of Yba 2 Cu 3 O 7−δ (YBCO) films grown by pulsed laser deposition on (100) SrTiO 3 (STO) and on rolling-assisted biaxially textured substrates (RABiTS). The thickness of YBCO films varied from 0.19 to 3 μm. The highest J c s of 5.3 and 2.6 MA/cm 2 at 77 K, self-field were obtained for 0.19-μm YBCO films on STO and RABiTS, respectively. J c was found to decrease exponentially with YBCO thickness on both substrates. However, the results suggest different mechanisms are responsible for the J c reduction in the two cases. On STO, growth of a -axis grains within c -axis films and broadening of the in-plane texture were observed in thick films. On RABiTS, degradation in cube texture as well as development of a porous surface morphology were found to correlate with film thickness.


Physica C-superconductivity and Its Applications | 2002

Strengthened, biaxially textured Ni substrate with small alloying additions for coated conductor applications

Amit Goyal; R. Feenstra; M. Paranthaman; J. R. Thompson; B.Y Kang; Claudia Cantoni; D.F. Lee; F.A. List; P.M. Martin; E Lara-Curzio; C Stevens; D. M. Kroeger; M. M. Kowalewski; Eliot D. Specht; Tolga Aytug; S. Sathyamurthy; R. K. Williams; R.E Ericson

Abstract Fabrication of a biaxially textured, strengthened Ni substrate with small alloying additions of W and Fe is reported. The substrates have significantly improved mechanical properties compared to 99.99% Ni and surface characteristics which are similar to that of 99.99% Ni substrates. High quality oxide buffer layers can be deposited on these substrates without the need for any additional surface modification steps. Grain boundary misorientation distributions obtained from the substrate show a predominant fraction of low-angle grain boundaries. A high critical current density, J c , of 1.9 MA/cm 2 at 77 K, self-field is demonstrated on this substrate using a multilayer configuration of YBCO/CeO 2 /YSZ/Y 2 O 3 / Ni–3at.%W–1.7at.%Fe. This translates to a I c /width of 59 A/cm at 77 K and self-field. J c at 0.5 T is reduced by only 21% indicating strongly-linked grain boundaries in the YBCO film on this substrate.

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M. Paranthaman

Oak Ridge National Laboratory

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Amit Goyal

Oak Ridge National Laboratory

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D. K. Christen

Oak Ridge National Laboratory

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D. M. Kroeger

Oak Ridge National Laboratory

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Eliot D. Specht

Oak Ridge National Laboratory

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D.F. Lee

Oak Ridge National Laboratory

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F.A. List

Oak Ridge National Laboratory

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Tolga Aytug

Oak Ridge National Laboratory

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Keith J. Leonard

Oak Ridge National Laboratory

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