Relevant bibliographies by topics / Superconducting multilayers

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  1. Journal articles
  2. Dissertations / Theses
  3. Books
  4. Book chapters
  5. Conference papers
  6. Reports

Academic literature on the topic 'Superconducting multilayers'

Author: Grafiati
Published: 4 June 2021
Last updated: 12 February 2022

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Journal articles on the topic "Superconducting multilayers"

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Sidorenko, A. S. "Superconducting Fractal Multilayers." Fractals 05, supp02 (October 1997): 101–17. http://dx.doi.org/10.1142/s0218348x97000851.

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The influence of fractal geometry on superconductivity has been studied for layered superconductors. Superconducting multilayers consisting of alternating Nb and Cu layers with fractal stacking sequence and fractal dimension Df=0.63 including the two limiting cases Df= 0 (single superconducting film) and Df=1 (periodic multilayers) were prepared by electron-beam evaporation in ultrahigh vacuum. The layers of Nb and Cu were put down alternately via computer control of the target shutter. The structure of the samples has been checked with in situ reflection high-energy electron diffraction (RHEED) and Auger depth profiling, confirmed the prescribed layering geometry. Superconductivity was investigated by measurements of the critical temperature of superconducting transition Tc, and of the temperature and of the angular dependence of the upper critical magnetic fields Bc2. The observed dependences of Tc on the parameters of fractal samples are in a good qualitative agreement with the proximity effect theory developed for layered superconductors with a self-similar fractal structure. The behavior of the upper critical magnetic field is directly related to the type of the layering. At low temperatures, all samples show the same two-dimensional behavior essentially governed by the topological dimension of the individual superconducting layers, independent of the fractal dimensionality Df of the samples, whereas for temperatures near Tc the type of layering determines the dimensionality, resulting in a multicrossover behavior of fractal samples. The angular dependence of the upper critical magnetic field Bc2(θ) of fractals corresponds to the theory for a two-dimensional superconductor at all temperatures, reflecting the multicrossover behavior of the fractal multilayers, as long as the temperature-dependent coherence length is comparable with a certain scale of fractal.
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Hegde, M. S., K. M. Satyalakshmi, S. Sundar Manoharan, and Dhananjay Kumar. "Superconducting and non-superconducting oxide multilayers." Materials Science and Engineering: B 32, no. 3 (July 1995): 239–45. http://dx.doi.org/10.1016/0921-5107(95)80026-3.

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Attanasio, C., L. Maritato, B. Engel, and C. M. Falco. "Superconducting spin-glass multilayers." Physica B: Condensed Matter 194-196 (February 1994): 1721–22. http://dx.doi.org/10.1016/0921-4526(94)91360-9.

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Song, S. N., B. Y. Jin, F. L. Du, and J. B. Ketterson. "Superconducting tunneling through multilayers." Superlattices and Microstructures 3, no. 5 (January 1987): 485–91. http://dx.doi.org/10.1016/0749-6036(87)90229-1.

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Tachiki, Masashi, and Saburo Takahashi. "Theory of superconducting multilayers." Physica C: Superconductivity 153-155 (June 1988): 1702–7. http://dx.doi.org/10.1016/0921-4534(88)90457-1.

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Nastasi, M., P. N. Arendt, R. Tesmer, C. J. Maggiore, R. C. Cordi, D. L. Bish, J. D. Thompson, et al. "Fabrication of oxide superconductors from multilayered metallic thin films." Journal of Materials Research 2, no. 6 (December 1987): 726–31. http://dx.doi.org/10.1557/jmr.1987.0726.

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Thin-film GdBa2Cu3Ox superconductors with an onset Tc > 90 K have been produced. The films were fabricated by thermal reaction in an oxidizing atmosphere of electron-beam deposited Ba/Gd/Cu multilayers. Attempts to produce the superconducting phase YBa2Cu3Ox by multilayer reaction were unsuccessful due to a positive heat of mixing between Y and Ba. The appearance of a wide superconducting transition in GdBa2Cu3Ox films may be the result of tunneling through a nonsuperconducting second phase.
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Plehn, H., O. J. Wacker, and R. Kümmel. "Electronic structure of superconducting multilayers." Physical Review B 49, no. 17 (May 1, 1994): 12140–50. http://dx.doi.org/10.1103/physrevb.49.12140.

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Takahashi, S., T. Hirai, M. Machida, and M. Tachiki. "Phase diagram in superconducting multilayers." Physica C: Superconductivity 235-240 (December 1994): 2585–86. http://dx.doi.org/10.1016/0921-4534(94)92513-5.

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Aarts, J., J. Meiressonne, H. Sprey, W. Maj, and P. Zagwijn. "Proximity effect in superconducting multilayers." Vacuum 41, no. 4-6 (January 1990): 1476–80. http://dx.doi.org/10.1016/0042-207x(90)93995-u.

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WANG, H. F., Y. Z. ZHANG, L. H. LIU, D. P. LI, G. Y. WANG, H. Y. TIAN, and D. N. ZHENG. "TRANSPORT PROPERTIES OF La2-x1Srx1CuO4+δ/La2-x2Srx2CuO4+δ MULTILAYERS GROWN BY LASER ABLATION." International Journal of Modern Physics B 27, no. 15 (June 4, 2013): 1362029. http://dx.doi.org/10.1142/s0217979213620294.

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A series of La 2-x1 Sr x1 CuO 4+δ/ La 2-x2 Sr x2 CuO 4+δ multilayers were epitaxially grown on (001) LaSrAlO 4 and (001) SrTiO 3 substrates by laser ablation, where x1 = 0.0, 0.08 (underdoped) and x2 = 0.24, 0.32, 0.45 (over-doped). Before the depositions of each multilayer, all of the single layers were deposited and characterized, and then the multilayers were deposited by using the same deposition condition except shifting targets for laser ablation. These multilayers are highly c-axis oriented. Several modulation wavelengths of the sublayers were selected for preparing the multilayers. The resistance measurements of these single layered films of La 2-x1 Sr x1 CuO 4+δ, La 2-x2 Sr x2 CuO 4+δ, and multilayers of La 2-x1 Sr x1 CuO 4+δ/ La 2-x2 Sr x2 CuO 4+δ were performed and compared. The transport measurements suggest that the charge redistribution may be a dominant factor for the superconducting transition temperature in low temperatures.
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Dissertations / Theses on the topic "Superconducting multilayers"

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Sadki, El Hadi Smail. "Vortex matter in low temperature superconducting multilayers." Thesis, University of Cambridge, 2002. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.620238.

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Kryukov, Sergiy A. "MAGNETIC PROPERTIES OF Nb/Ni SUPERCONDUCTING / FERROMAGNETIC MULTILAYERS." UKnowledge, 2012. http://uknowledge.uky.edu/physastron_etds/7.

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Magnetic properties of Nb/Ni superconducting (SC) / ferromagnetic (FM) multilayers exhibit interesting properties near and below SC transition. A complex Field (H) – Temperature (T) phase boundary is observed in perpendicular and parallel orientation of ML with respect to DC field. We address the critical need to develop methods to make reliable magnetic measurements on SC thin films and ML, in spite of their extreme shape anisotropy and the strong diamagnetic response of the SC state. Abrupt, highly reproducible “switching” of the SC state magnetization near the normal-state FM coercive fields has been observed in Nb/Ni ML. The SC penetration depth l(Nb) > the SC coherence length xo(Nb) » 40 nm >> the FM layer thickness y(Ni) = 5 nm, abrupt magnetic reversals might be driven by strong supercurrent densities (J x M torques) that have the potential to flow into the Ni layers. Alternatively, sharp magnetization anomalies also can result from strong flux pinning by the periodic layered structure of ML, including “lock-in” of quantized flux lines (FL) parallel to the ML plane. Strong confinement of the supercurrents within ML planes might also lead to various phase transitions of the FL lattice (FLL) composed of one-dimensional chains and other unusual structures. Possible mechanisms for the switching anomalies must be evaluated while considering other experimental properties of Nb(x)/Ni(y) ML: 1) The upper critical magnetic field Hc2(T) exhibits a highly unusual anisotropy where the SC transition temperature Tc (H®0) for DC field H ^ ML plane exceeds the value for H || ML by ~ 0.5 K. 2) Nb/Ni ML samples do not consistently exhibit magnetic signatures for the onset of superconductivity, depending on the details of the sample mounting procedure and the AC or DC method used in SQUID magnetometry experiments. 3) Unusual “wiggles” or oscillations of order 10-30 mK were observed in Hc2(T) in AC SQUID experiments with H || ML and can be even larger (~0.16 K), depending upon the AC drive amplitude ho and frequency f .
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Wong, André Wing Gai. "Ion implantation patterning of high temperature superconducting thin films and multilayers." Thesis, National Library of Canada = Bibliothèque nationale du Canada, 1999. http://www.collectionscanada.ca/obj/s4/f2/dsk1/tape9/PQDD_0001/NQ39005.pdf.

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LIU, LIYING. "EFFECT OF INTERFACE ROUGHNESS AND HEAT-TREATMENT OF THE SUPERCONDUCTING PROPERTIES OF NB/CO MULTILAYERS." PONTIFÍCIA UNIVERSIDADE CATÓLICA DO RIO DE JANEIRO, 2012. http://www.maxwell.vrac.puc-rio.br/Busca_etds.php?strSecao=resultado&nrSeq=20721@1.

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PONTIFÍCIA UNIVERSIDADE CATÓLICA DO RIO DE JANEIRO
Neste trabalho foram preparadas multi-camadas supercondutor(SC)/ ferromagneto(FM) Nb/Co via pulverização catódica (Magnetron Sputtering). O principal objetivo é estudar o efeito de diferentes espessuras da camada ferromagnética (Co) nas propriedades supercondutoras do Nb. Era esperado que, após tratamentos térmicos, as camadas de Co formassem um plano de nanopartículas magnéticas ordenadas, cujo efeito deve ser muito diferente das nanopartículas aleatoriamente orientadas e camadas magnéticas continuas. As microestruturas foram investigadas por Difração de Raios-X em baixos ângulos (LAXRD), Microscopia de Força Atômica (AFM) e Microscopia Eletrônica de Transmissão (TEM). Propriedades magnéticas e de transporte tem sido estudadas com o Sistema de Medição de Propriedade Físicas (PPMS), da empresa Quantum Design. As medidas magnéticas e de transporte mostram que, com o aumento da espessura das camadas de Co, a temperatura de transição supercondutora (Tc) aumenta significativamente para as amostras como preparadas. Foi relatado na literatura que quando a espessura das camadas magnéticas da ordem de alguns nanômetros, a Tc aumenta e diminui periodicamente com o aumento da espessura das camadas magnéticas. No entanto, nesta pesquisa, a espessura das camadas magnéticas é de dezenas de nanômetros, sendo muito maior do que este alcance e portanto, não pode ser explicado baseando-se no mesmo modelo. Propusemos que a rugosidade da interface entre as camadas de Co e Nb desempenha um papel importante para este comportamento. Os resultados de AFM e XRD mostram que a rugosidade máxima da interface é da ordem de 7 a 10 nm, o que é comparável à espessura de camadas de Co (de 5 a 20 nm). Introduzimos um parâmetro R igual a d, onde R é a rugosidade da interface e d é a espessura da camada magnética, para discutir o efeito da interface sobre as propriedades supercondutoras da nossa amostra. Quando delta maior que 1, a camada magnética pode ser considerada uma forma não-continua e somente quando delta menor que 1, as camadas magnéticas continuas podem ser formadas. Com base em observações de topografia de interfaces na nano-escala , podemos compreender que primeiro a rugosidade aumenta a área da interface, resultando em um efeito de proximidade mais forte, além de aumentar o efeito do campo de dispersão na Tc. Este efeito depende não somente da rugosidade, mas também da espessura da camada magnética. Verificou-se que o parâmetro determina o efeito das camadas magnéticas. As diferentes propriedades magnéticas abaixo da Tc para diferentes amostras também pode ser explicada por este modelo. Após o tratamento térmico, a Tc das amostras diminuiu e as propriedades magnéticas também se tornam piores do que as amostras como preparadas. Os resultados de TEM mostram que as camadas de Co estam interconectadas e depois do recozimento não há indícios de interdifusão entre as camadas Nb e Co. Mais medidas são necessárias para verificar se as camadas magnéticas podem induzir vórtices espontâneos, assim como para explicar a diferença entre as amostras com nanopartículas magnéticas ordenadas comparadas com aquelas orientadas aleatoriamente.
In this work we prepared Superconductor(SC)/ferromagnet(FM) Nb/Co multi-layers with magnetron-sputtering. The main purpose of this work is to study the effect of different shape of ferromagnetic layers on the superconducting properties of Nb. We expected that after annealing the Co layers can form in-plane ordered magnetic nanoparticles and the effect of ordered magnetic nanoparticles should be very different from randomly oriented nanoparticles and continues magnetic layers. The microstructures have been investigated by means of Low Angle X-ray Diffraction (LAXRD), Atomic Force Microscopy (AFM) and Transmission Electron Microscopy (TEM). Magnetic and transport properties have been studied with Physical Property Measurement System (PPMS) from Quantum Design. The magnetic and transport measurements show that with increase of the thickness of Co layers the superconducting transition temperature (Tc) signifficantly increases for the as-prepared samples. It was reported in the literature that when the thickness of the magnetic layers is in the range of several nanometers, Tc increases and decreases periodically with the increase of the thickness of the magnetic layers. In our samples, however, the thickness of the magnetic layers (several tens nanometers) is much larger than that range and therefore, cannot be explained within the same model. We proposed that the roughness of the interface between Co and Nb layers plays an important role for this behavior. The AFM and LAXRD results show that the maxim roughness of the interface is in the range of 7 until 10 nm, which is comparable to the thickness of Co layers (5 until 20 nm). We introduced one parameter R equal d, where R is the roughness of the interface and d is the thickness of the magnetic layer, to discuss the effect of the interface on the superconducting properties of our sample. When delta more 1, the magnetic layer may be in a non-continues form and only when delta less1 continues magnetic layers can be formed. Based upon nano-scale observations of interfaces topography we can understand that the roughness first increases the area of the interface, which gives stronger proximity effect and, second, enhances the effect of the stray eld on Tc. This effect depends not only the roughness but also the thickness of the magnetic layer. It was found out that the parameter determines the effect of the magnetic layers. The different magnetic properties below Tc for different samples can also be explained by this model. After annealing, Tc of the samples decreased and magnetic properties also became worse than the as-prepared samples. The TEM results show that the Co layers is interconnected and after annealing there is no indication of interdiffusion between Nb and Co layers. More measurements are needed to see if the magnetic layers can induce spontaneous vortices and what the difference is between samples with ordered and randomly oriented magnetic nano-particles.
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SANTOS, Flávia Portela. "Estudo das propriedades supercondutoras em multicamadas de Nb, Pb, e Sn." Universidade Federal de Pernambuco, 2015. https://repositorio.ufpe.br/handle/123456789/17342.

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O estudo em sistemas de multicamadas supercondutoras alcan cou grande interesse na pesquisa de novos materiais, pois al em de apresentarem ampla aplicabilidade tecnol ogica, oferecem fascinantes possibilidades de observar novos fen^omenos na supercondutividade. Esta ultima caracter stica e a de maior motiva c~ao para esta tese, uma vez que pouco ainda se tem reportado a respeito da supercondutividade em multicamadas constitu das por supercondutor(S)/supercondutor(S0). Neste trabalho, estudamos tr^es novos sistemas nanoestruturados formados por supercondutores elementares, de baixa temperatura cr tica, tais como ni obio (Nb), chumbo (Pb) e estanho (Sn), a saber, a tricamada Nb(5)/Pb(500)/Nb(50) e as multicamadas Nb(100)/[Sn(50)/Nb(50)]7 e Cr(10)/Nb(100)/[Sn(50)/Nb(50)]7, onde o termo entre par^enteses indica a espessura da referida camada em nan^ometros e os colchetes indicam que a estrutura Nb/Sn e repetida 7 vezes. Para compara c~ao, tamb em s~ao analisados lmes de refer^encia de Nb, Pb e Sn. Os lmes e as multicamadas foram crescidos a temperatura ambiente por deposi c~ao via sputtering, utilizando fontes DC e RF. As amostras foram caracterizadas por difra c~ao de raios X de baixo ^angulo, microscopia eletr^onica de varredura e por microscopia de for ca at^omica. As propriedades supercondutoras foram estudadas atrav es de medidas magn eticas e de transporte el etrico. Magnetiza c~ao e resistividade foram medidas como fun c~oes da temperatura e do campo magn etico aplicado perpendicular e paralelamente as camadas. Os tr^es sistemas apresentaram transi c~oes supercondutoras abruptas, tanto na magnetiza c~ao quanto na resistividade em fun c~ao da temperatura, com os valores de TC obtidos de 7,2 K para o Nb/Pb/Nb, 5,2 K para o Nb/[Sn/Nb]7 e 3,7 K para o Cr/Nb/[Sn/Nb]7. As propriedades supercondutoras dos lmes de Pb, Nb e Sn, tais como TC, 0Hc2 e comprimentos caracter sticos apresentaram coer^encia com os valores reportados na literatura, con rmando a boa qualidade das camadas. Flux jumps s~ao observados nos loops de histerese em todos os sistemas, os quais s~ao atribu dos a instabilidades termomagn eticas. A amostra Nb/Pb/Nb apresentou uma curvatura positiva na depend^encia de 0Hc2(T), indicando que a supercondutividade ocorre preferencialmente na camada de Pb para T > T e preferencialmente na camada de Nb para T < T , de acordo com a teoria de Takahashi-Tachiki. Os comprimentos caracter sticos s~ao calculados, classi cando as multicamadas como supercondutores do tipo II. Veri camos grande in u^encia do material magn etico Cr na supercondutividade da multicamada, causando a diminui c~ao da temperatura cr tica do sistema e modi cando o comportamento dos campos cr ticos inferior e superior. A depend^encia de 0Hc1(T), em todos os sistemas, revelou um comportamento n~ao convencional, que e atribu do a uma manifesta c~ao de sistemas multicomponentes com componentes espacialmente separadas.
The study of superconducting multilayers systems has achieved much interest in the research of new materials. Besides their wide technological applicability, these structures o er fascinating possibilities to observe new phenomena in superconductivity. The latter characteristic is the fundamental motivation for this thesis, since a little has been reported about multilayers constituted of superconductor(S)/superconductor(S0). In this work, we have studied three new nanostructured systems formed by low critical temperature conventional superconductors, such as niobium (Nb), lead (Pb) and tin (Sn): the trilayer Nb(5)/Pb(500)/Nb(50) and the multilayers Nb(100)/[Sn(50)/Nb(50)]7 and Cr(10)/Nb(100)/[Sn(50)/Nb(50)]7. The term in parenthesis indicates the thickness of the layer in nanometers and the brackets that Nb/Sn structure is repeated 7 times. For comparison, the reference lms of Nb, Pb and Sn were also analyzed. The thin lms and multilayers were growth at room temperature via sputtering deposition, by using DC and RF sources. The samples were characterized for small angle X ray di raction, scanning electron microscopy (SEM), and atomic force microscopy (AFM). The superconducting properties were investigated through magnetic and electric transport measurements. The magnetization and resistivity were obtained as functions of temperature and magnetic eld applied both perpendicularly and parallel to the layers. All the multilayers systems have showed sharp superconducting transitions in the dependence of magnetization and resistivity with the temperature. The multilayers critical temperatures were found to be 7.2 K for Nb/Pb/Nb, 5.2 K for Nb/[Sn/Nb]7 and 3.7 K for Cr/Nb/[Sn/Nb]7. The superconducting properties of reference lms Pb, Nb and Sn, such as critical temperature, upper critical eld and characteristic lengths were consistent with the literature values, con rming the good quality of the samples. In the three systems ux jumps were observed, which are attributed to thermomagnetic instabilities. The Ginzburg-Landau parameter is estimated, classifying the multilayers as type II superconductors. In the case of Nb/Pb/Nb sample, it presented an upward curvature in the 0Hc2(T) diagrams, which is a signature of superconductivity nucleation in the each layer, in accordance with Takahashi-Tachiki theory for multilayered systems. We found out a noticeable in uence of the magnetic material Cr on the multilayer superconducting properties, reducing the critical temperature of the system and modifying the lower and upper critical elds behavior. The dependence of 0Hc1(T), of all the multilayers, revealed a non-conventional behavior feature, which is consistent with a multicomponent behavior with spatially separated components.
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Li, Quan. "AC loss characteristics of monolayer and multilayer superconducting power transmission cables." Thesis, University of Cambridge, 2011. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.609500.

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Yi, Ge. "Single-crystal superconducting Pb nanowires and nanostructures." Thesis, University of Bristol, 1999. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.266955.

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楊曄 and Ye Yang. "Microstructure characterization of high Tc superconducting thin films and multilayer Josephson junctions." Thesis, The University of Hong Kong (Pokfulam, Hong Kong), 1998. http://hub.hku.hk/bib/B31220186.

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Yang, Ye. "Microstructure characterization of high Tc superconducting thin films and multilayer Josephson junctions /." Hong Kong : University of Hong Kong, 1998. http://sunzi.lib.hku.hk/hkuto/record.jsp?B19471099.

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Zhao, Yue. "Fabrication and characterization of superconducting PLD MgB2 thin films." Access electronically, 2005. http://www.library.uow.edu.au/adt-NWU/public/adt-NWU20060719.121046/index.html.

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Books on the topic "Superconducting multilayers"

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Ivan, Bozovic, and Society of Photo-optical Instrumentation Engineers., eds. Superconducting superlattices and multilayers: 24-25 January 1994, Los Angeles, California. Bellingham, Wash., USA: SPIE, 1994.

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Book chapters on the topic "Superconducting multilayers"

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Attanasio, C., C. Coccorese, L. Maritato, I. Mercaldo, and M. Salvato. "Superconducting Properties of Nb/CuMn Multilayers." In Fluctuation Phenomena in High Temperature Superconductors, 415–23. Dordrecht: Springer Netherlands, 1997. http://dx.doi.org/10.1007/978-94-011-5536-6_35.

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Haindl, Silvia. "More Interfaces: Multilayers and Heterostructures with Fe-Based Superconductors." In Iron-Based Superconducting Thin Films, 235–52. Cham: Springer International Publishing, 2021. http://dx.doi.org/10.1007/978-3-030-75132-6_5.

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Miura, Masashi. "Nanostructured Oxide Superconducting Films Prepared by Metal Organic Deposition." In Oxide Thin Films, Multilayers, and Nanocomposites, 3–26. Cham: Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-14478-8_1.

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Kaneko, Satoru, Uli Hiller, Jon M. Slaughter, Charles M. Falco, Corrado Coccorese, and Luigi Maritato. "Structure and Superconducting Properties of Nb/Pd Multilayers." In Advances in Superconductivity XI, 1137–40. Tokyo: Springer Japan, 1999. http://dx.doi.org/10.1007/978-4-431-66874-9_267.

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Miryala, Santosh. "Design and Development of High-T c Superconducting Train Model Using Bulk Nanocomposite GdBa2Cu3O y." In Oxide Thin Films, Multilayers, and Nanocomposites, 97–106. Cham: Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-14478-8_6.

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Hidaka, Hiroaki, and Hiroshi Yamamura. "The Stress-Strain Relationship for Multilayers of the High Tc Superconducting Oxides." In Advances in Superconductivity, 581–86. Tokyo: Springer Japan, 1989. http://dx.doi.org/10.1007/978-4-431-68084-0_98.

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Nojima, Tsutomu, Masayuki Kinoshita, Yoshinori Kuwasawa, and Shigeru Nakano. "Anisotropy of Critical Current and 2D Mixed State in Superconducting Nb/NbZr Multilayers." In Advances in Superconductivity V, 497–500. Tokyo: Springer Japan, 1993. http://dx.doi.org/10.1007/978-4-431-68305-6_111.

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Singh, Shiv Jee, Muralidhar Miryala, and Paolo Mele. "Fabrication of (Nd0.33Eu0.33Gd0.33)Ba2Cu3Oy Superconducting Thin Films by Pulsed Laser Ablation of Melt-Textured Targets." In Surfaces and Interfaces of Metal Oxide Thin Films, Multilayers, Nanoparticles and Nano-composites, 223–32. Cham: Springer International Publishing, 2021. http://dx.doi.org/10.1007/978-3-030-74073-3_10.

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Borukhovich, Arnold S., and Alexey V. Troshin. "Creation and Research of Properties of Multilayers and Superconducting Tunnel Transitions with the Participation of EuO." In Europium Monoxide, 121–38. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-76741-3_5.

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Witanachchi, S., D. T. Shaw, H. S. Kwok, E. Narumi, Y. Z. Zhu, and S. Patel. "Multilayer Flexible Oxide Superconducting Tapes." In Superconductivity and Applications, 665–75. Boston, MA: Springer US, 1990. http://dx.doi.org/10.1007/978-1-4684-7565-4_66.

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Conference papers on the topic "Superconducting multilayers"

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Ruck, Ben J., S. Brown, and H. J. Trodahl. "Superconducting properties of Ta/Ge multilayers." In Photonics West '96, edited by Ivan Bozovic and Davor Pavuna. SPIE, 1996. http://dx.doi.org/10.1117/12.250278.

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Narumi, E., J. Lee, S. Patel, and D. T. Shaw. "Superconducting behavior of YBa2Cu3O6.8/Bi2Sr2CanCun+1 multilayers." In Superconductivity and its applications. AIP, 1992. http://dx.doi.org/10.1063/1.43605.

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Zhao, Bai Ru, B. T. Liu, Yingzhang Lin, Z. Hao, E. Z. Luo, Z. Xie, I. H. Wilson, and B. Xu. "Growth and features of high-T c superconducting multilayers and heterostructures." In SPIE's International Symposium on Optical Science, Engineering, and Instrumentation, edited by Ivan Bozovic and Davor Pavuna. SPIE, 1998. http://dx.doi.org/10.1117/12.332441.

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Takahashi, Saburo, Toshio Hirai, and Masashi Tachiki. "Mechanism for the peak effect of critical current in superconducting multilayers." In OE/LASE '94, edited by Ivan Bozovic. SPIE, 1994. http://dx.doi.org/10.1117/12.179154.

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Kuwasawa, Yoshinori, Tsutomu Nojima, Eisaku Touma, Masaki Fukuhara, and Shigeru Nakano. "Influence of crystalline orientation on the superconducting properties in V/Cr-multilayers." In OE/LASE '94, edited by Ivan Bozovic. SPIE, 1994. http://dx.doi.org/10.1117/12.179164.

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Bruynseraede, Yvon, Vitaly V. Metlushko, K. Temst, M. Baert, E. Rosseel, M. J. Van Bael, and Victor V. Moshchalkov. "Confinement of the flux-line lattice in nanostructured superconducting films and multilayers." In Photonics West '96, edited by Ivan Bozovic and Davor Pavuna. SPIE, 1996. http://dx.doi.org/10.1117/12.250246.

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Lomatch, Susanne. "Theory and application of Josephson-coupled multilayers as switching devices in superconducting electronics." In SPIE's International Symposium on Optical Science, Engineering, and Instrumentation, edited by Ivan Bozovic and Davor Pavuna. SPIE, 1998. http://dx.doi.org/10.1117/12.332460.

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Mercaldo, Lucia V., Carmine Attanasio, and Luigi Maritato. "Systematic analysis of the critical temperature oscillations in superconducting (Nb)/spin-glass (CuMn) multilayers." In SPIE's International Symposium on Optical Science, Engineering, and Instrumentation, edited by Ivan Bozovic and Davor Pavuna. SPIE, 1998. http://dx.doi.org/10.1117/12.332446.

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Braccini, Valeria, Daniele Marre, Giuseppe Grassano, and Antonio S. Siri. "Superconducting artificial multilayers based on (Ba,Ca)/CuO 2 grown by pulsed laser ablation." In AeroSense 2000, edited by Davor Pavuna and Ivan Bozovic. SPIE, 2000. http://dx.doi.org/10.1117/12.397859.

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Gray, Kenneth E., J. F. Hettinger, and Dennis Kim. "Effects of interlayer coupling on the magnetic and transport properties of superconducting multilayers and high-temperature superconductors." In OE/LASE '94, edited by Ivan Bozovic. SPIE, 1994. http://dx.doi.org/10.1117/12.179151.

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Reports on the topic "Superconducting multilayers"

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Gonczy, J., W. Boroski, and R. Niemann. Multilayer Insulation (Mli) in the Superconducting Super Collider: A Practical Engineering Approach to Physical Parameters Governing Mli Thermal Performance. Office of Scientific and Technical Information (OSTI), March 1989. http://dx.doi.org/10.2172/1151491.

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Whitlow, G., J. Bowker, W. Lovic, F. List, and D. Kroeger. High critical current silver-Bi{sub 2}Sr{sub 2}CaCu{sub 2}O{sub 8{minus}x} superconducting multilayer ribbons produced by rolling. Office of Scientific and Technical Information (OSTI), December 1992. http://dx.doi.org/10.2172/10119506.

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