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Journal articles on the topic 'Superconductor Quantum Interference Device'

Author: Grafiati

Published: 4 June 2021

Last updated: 10 February 2022

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1

Hammad, Fayçal, and Alexandre Landry. "A simple superconductor quantum interference device for testing gravity." Modern Physics Letters A 35, no. 20 (2020): 2050171. http://dx.doi.org/10.1142/s0217732320501710.

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A simple tabletop setup based on a superconductor quantum interference device is proposed to test the gravitational interaction. A D-shaped superconducting loop has the straight segment immersed inside a massive sphere while the half-circle segment is wrapped around the sphere. The superconducting condensate within the straight arm of the loop thus bathes inside a gravitational simple harmonic oscillator potential while the condensate in the half-circle arm bathes in the constant gravitational potential around the sphere. The resulting phase difference at the Josephson junctions on both sides

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2

Bagani, Kousik. "Scanning SQUID-on-tip Magnetic and Thermal Microscopy." Science Dialectica 01, no. 1 (2021): 1–3. http://dx.doi.org/10.54162/sd01-25201/01.

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Scanning magnetic and thermal imaging using Superconducting Quantum Interference Device (SQUID) fabricated on the apex of a sharp tip has attracted great attention because of its record magnetic sensitivity, thermal sensitivity and nanoscale spatial resolution. Many interesting phenomena like vortex dynamics in a superconductor, quantum hall state, and heat dissipation in graphene etc. has been investigated using scanning SQUID on tip microscopy. This is one of the most powerful tool for the investigation of a wide variety of quantum systems and novel materials.

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3

Lin, Jianxin, Benedikt Müller, Julian Linek, et al. "YBa2Cu3O7 nano superconducting quantum interference devices on MgO bicrystal substrates." Nanoscale 12, no. 9 (2020): 5658–68. http://dx.doi.org/10.1039/c9nr10506a.

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4

Takagi, Ryuki, Mohd Mawardi Saari, Kenji Sakai, Toshihiko Kiwa, and Keiji Tsukada. "Compact AC/DC Susceptometer using a High-temperature Superconductor Superconducting Quantum Interference Device." IEEJ Transactions on Fundamentals and Materials 134, no. 6 (2014): 369–74. http://dx.doi.org/10.1541/ieejfms.134.369.

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5

Veauvy, C., K. Hasselbach та D. Mailly. "Scanning μ-superconduction quantum interference device force microscope". Review of Scientific Instruments 73, № 11 (2002): 3825–30. http://dx.doi.org/10.1063/1.1515384.

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6

Zhou, Ji Ping, John T. McDevitt, and Q. X. Jia. "Improved N-layer materials for high-Tc superconductor/normal-metal/superconductor junctions and superconducting quantum interference device sensors." Applied Physics Letters 72, no. 7 (1998): 848–50. http://dx.doi.org/10.1063/1.120913.

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7

He, D. F., M. Yoshizawa, and M. Nakamura. "Mobile high-temperature superconductor dc superconducting quantum interference device cooled by a pulse-tube cooler." Review of Scientific Instruments 76, no. 7 (2005): 074704. http://dx.doi.org/10.1063/1.1946927.

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8

Li, Mary J., S. Aslam, T. C. Chen, et al. "Interfacial And Surface Study Of Mo-Au And Al-Ag Bilayers For Si-Based Photodetectors." Microscopy and Microanalysis 5, S2 (1999): 164–65. http://dx.doi.org/10.1017/s1431927600014148.

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Bilayer thin films have been utilized in superconducting transition-edge sensors (TES) for photodetector development. A TES is formed with a normal metal conductor film and a superconductor film, so called bilayer, deposited on a subtract. In its,transition temperature region, the resistance of the superconductor film is extremely sensitive to the temperature. When an incident radiation ray arrives, the temperature of the bilayer increases, leading the resistance increases tremendously. A superconducting quantum interference device measures the current variation for read-out. By varying the re

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9

Takeda, Keiji, Hatsumi Mori, Akira Yamaguchi, et al. "High temperature superconductor micro-superconducting-quantum-interference-device magnetometer for magnetization measurement of a microscale magnet." Review of Scientific Instruments 79, no. 3 (2008): 033909. http://dx.doi.org/10.1063/1.2894332.

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10

Lee, Soon-Gul, Yunseok Hwang, Byung-Chang Nam, Jin-Tae Kim, and In-Seon Kim. "Direct-coupled second-order superconducting quantum interference device gradiometer from single layer of high temperature superconductor." Applied Physics Letters 73, no. 16 (1998): 2345–47. http://dx.doi.org/10.1063/1.122456.

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11

Takeda, Keiji, Hatsumi Mori, Akira Yamaguchi, et al. "Fabrication of a high temperature superconductor micro-superconducting-quantum-interference-device magnetometer for magnetic hysteresis measurements." Journal of Applied Physics 103, no. 7 (2008): 07E911. http://dx.doi.org/10.1063/1.2835477.

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12

Jia, Q. X., D. Reagor, C. Mombourquette, Y. Fan, J. Decker, and P. D’Alessandris. "Stability of dc superconducting quantum interference devices fabricated using ramp-edge superconductor/normal-metal/superconductor technology." Applied Physics Letters 71, no. 12 (1997): 1721–23. http://dx.doi.org/10.1063/1.120015.

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13

Merkle, K. L., and Y. Huang. "Microstructure of Josephson Junctions: Effect on Supercurrent Transport in YBCO Grain Boundary and Barrier Layer Junctions." Microscopy and Microanalysis 4, S2 (1998): 792–93. http://dx.doi.org/10.1017/s1431927600024089.

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The electric transport of high-temperature superconductors, such as YBa2Cu307-x (YBCO), can be strongly restricted by the presence of high-angle grain boundaries (GB). This weak-link behavior is governed by the macroscopic GB geometry and the microscopic grain boundary structure and composition at the atomic level. Whereas grain boundaries present a considerable impediment to high current applications of high Tc materials, there is considerable commercial interest in exploiting the weak-link-nature of grain boundaries for the design of microelectronic devices, such as superconducting quantum i

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14

Wolter, Silke, Julian Linek, Josepha Altmann, et al. "Fabrication Process for Deep Submicron SQUID Circuits with Three Independent Niobium Layers." Micromachines 12, no. 4 (2021): 350. http://dx.doi.org/10.3390/mi12040350.

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We present a fabrication technology for nanoscale superconducting quantum interference devices (SQUIDs) with overdamped superconductor-normal metal-superconductor (SNS) trilayer Nb/HfTi/Nb Josephson junctions. A combination of electron-beam lithography with chemical-mechanical polishing and magnetron sputtering on thermally oxidized Si wafers is used to produce direct current SQUIDs with 100-nm-lateral dimensions for Nb lines and junctions. We extended the process from originally two to three independent Nb layers. This extension offers the possibility to realize superconducting vias to all Nb

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15

Kandori, Akihiko, Kuniomi Ogata, Ryuzo Kawabata, Sayaka Tanimoto, and Yusuke Seki. "Note: Low temperature superconductor superconducting quantum interference device system with wide pickup coil for detecting small metallic particles." Review of Scientific Instruments 83, no. 7 (2012): 076108. http://dx.doi.org/10.1063/1.4739311.

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16

Hwang, Seong-min, Kiwoong Kim, Kwon Kyu Yu, et al. "Type-I superconductor pick-up coil in superconducting quantum interference device-based ultra-low field nuclear magnetic resonance." Applied Physics Letters 104, no. 6 (2014): 062602. http://dx.doi.org/10.1063/1.4865497.

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17

Astuti, Fahmi, Malik Anjelh Baqiya та Darminto. "Effect of Pb Substitution on Superconducting and Normal State Electrical Properties of Bi₂Sr₂CaCu₂O_8+σ Nanopowders". Materials Science Forum 827 (серпень 2015): 235–39. http://dx.doi.org/10.4028/www.scientific.net/msf.827.235.

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Abstract.The powders of Bi2-xPbxSr2CaCu2O8+δ(x=0; 0.4) superconductor have been prepared by using dissolved method followed by short period of sintering and calcination process . The purpose of this research is to study about the Pb doped effect to the properties of BSCCO nanopowders especially in the electric and superconducting properties. Based on the previous result, BSCCO nanopowders have ferromagnetic properties at the room temperature. This characteristic is not appeared in bulk superconductor. The 2212 phase of Bi-based system has been formed and observed by using X-ray diffraction (XR

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18

Huang, Y., L. Lee, M. Teepe, K. L. Merkle, and K. Char. "Microstructure of Grain Boundary Junctions in Bicrystal High-Tc Superconductor SQUIDs and its Relation with the Device Noise." Microscopy and Microanalysis 3, S2 (1997): 667–68. http://dx.doi.org/10.1017/s1431927600010229.

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Superconductor Quantum Interference Devices (SQUIDs), because of their extreme sensitivity to magnetic fields and radiation, have found important applications in biomagnetism, non-destructive evaluation and geophysics. One problem in the application of high-Tc SQUIDs is their noise performance. Recently, considerable progress has been made in reducing the noise. To understand the underlying mechanism, it is important to identify the microstructural origin of the junction noise.In this work actual SQUIDs of good and poor noise performance are studied and compared by TEM. The devices were made b

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19

Seredinski, Andrew, Anne Draelos, Ming-Tso Wei, et al. "Supercurrent in Graphene Josephson Junctions with Narrow Trenches in the Quantum Hall Regime." MRS Advances 3, no. 47-48 (2018): 2855–64. http://dx.doi.org/10.1557/adv.2018.469.

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ABSTRACTCoupling superconductors to quantum Hall edge states is the subject of intense investigation as part of the ongoing search for non-abelian excitations. Our group has previously observed supercurrents of hundreds of picoamperes in graphene Josephson junctions in the quantum Hall regime. One of the explanations of this phenomenon involves the coupling of an electron edge state on one side of the junction to a hole edge state on the opposite side. In our previous samples, these states are separated by several microns. Here, a narrow trench perpendicular to the contacts creates counterprop

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20

Hatsukade, Yoshimi, Makoto Takemoto, Ryuichi Kurosawa, and Saburo Tanaka. "Integrated High-Temperature Superconductor Radio-Frequency Superconducting Quantum Interference Device Covered with Superconducting Thin Films in Flip-Chip Configuration." Applied Physics Express 4, no. 6 (2011): 063101. http://dx.doi.org/10.1143/apex.4.063101.

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21

Muralidhar, M., M. Jirsa, N. Sakai, Y. Wu, and M. Murakami. "Magnetic and microstructure study of bulk (Sm0.33Eu0.33Gd0.33)Ba2Cu3Oy with submicron Gd2BaCuO5 second-phase particles." Journal of Materials Research 18, no. 5 (2003): 1073–80. http://dx.doi.org/10.1557/jmr.2003.0148.

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We fabricated melt-processed (Sm0.33Eu0.33Gd0.33)Ba2Cu3Oy superconductors with fine Gd2BaCuO5 (Gd-211) particles and studied microstructure and magnetic properties as a function of the Gd-211 content and the initial particle size. Microstructure observation by scanning electron microscopy and transmission electron microscopy confirmed the presence of submicron secondary-phase particles and nanometer-sized RE1+xBa2-xCu3Oy (x ≫ 0) clusters. At 77 K, the critical current densities of 107 and 83 kA/cm2 were achieved at 0 T (self-field) and 2.2 T, respectively (superconducting quantum interference

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22

Lesser, Omri, Andrew Saydjari, Marie Wesson, Amir Yacoby, and Yuval Oreg. "Phase-induced topological superconductivity in a planar heterostructure." Proceedings of the National Academy of Sciences 118, no. 27 (2021): e2107377118. http://dx.doi.org/10.1073/pnas.2107377118.

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Topological superconductivity in quasi-one-dimensional systems is a novel phase of matter with possible implications for quantum computation. Despite years of effort, a definitive signature of this phase in experiments is still debated. A major cause of this ambiguity is the side effects of applying a magnetic field: induced in-gap states, vortices, and alignment issues. Here we propose a planar semiconductor–superconductor heterostructure as a platform for realizing topological superconductivity without applying a magnetic field to the two-dimensional electron gas hosting the topological stat

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23

Nam, Hyoungdo, Hua Chen, Tijiang Liu, et al. "Ultrathin two-dimensional superconductivity with strong spin–orbit coupling." Proceedings of the National Academy of Sciences 113, no. 38 (2016): 10513–17. http://dx.doi.org/10.1073/pnas.1611967113.

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We report on a study of epitaxially grown ultrathin Pb films that are only a few atoms thick and have parallel critical magnetic fields much higher than the expected limit set by the interaction of electron spins with a magnetic field, that is, the Clogston–Chandrasekhar limit. The epitaxial thin films are classified as dirty-limit superconductors because their mean-free paths, which are limited by surface scattering, are smaller than their superconducting coherence lengths. The uniformity of superconductivity in these thin films is established by comparing scanning tunneling spectroscopy, sca

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24

Sugimoto, Akira, Ienari Iguchi, Takashi Miyake, and Hisashi Sato. "Diamagnetic Precursor State in High-Tc Oxide Superconductors near Optimal Doping Using Scanning Superconducting Quantum Interference Device Microscopy." Japanese Journal of Applied Physics 41, Part 2, No. 5A (2002): L497—L499. http://dx.doi.org/10.1143/jjap.41.l497.

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25

Lenk, Daniel, Vladimir I. Zdravkov, Jan-Michael Kehrle, et al. "Thickness dependence of the triplet spin-valve effect in superconductor–ferromagnet–ferromagnet heterostructures." Beilstein Journal of Nanotechnology 7 (July 4, 2016): 957–69. http://dx.doi.org/10.3762/bjnano.7.88.

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Background: In nanoscale layered S/F1/N/F2/AF heterostructures, the generation of a long-range, odd-in-frequency spin-projection one triplet component of superconductivity, arising at non-collinear alignment of the magnetizations of F1 and F2, exhausts the singlet state. This yields the possibility of a global minimum of the superconducting transition temperature T c, i.e., a superconducting triplet spin-valve effect, around mutually perpendicular alignment. Results: The superconducting triplet spin valve is realized with S = Nb a singlet superconductor, F1 = Cu41Ni59 and F2 = Co ferromagnetic

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26

Bondarenko, Stanislav, and Valentin Koverya. "Superconductivity in the Institute for Low Temperature Physics and Engineering of the National Academy of Sciences of Ukraine." International Journal of Modern Physics B 29, no. 25n26 (2015): 1542013. http://dx.doi.org/10.1142/s0217979215420138.

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The report contains a brief history of the superconductor’s researches and their applications carried out in the Institute for Low Temperature Physics and Engineering (ILTPE) of the National Academy of Sciences of Ukraine since the ILTPE foundation in 1960. The most important results of the researches in the field of the low- and high-temperature superconductors (HTS) are stated more detailed. The experimental validation of an electromagnetic radiation of Josephson junctions; the electron pairing and existence of the distant order in the HTS; a creation of the superconducting quantum interfere

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27

Wu, Chun Hua, Min Xu, Jie Bing Wang, Lin Li, Yin Zhong Zhao, and Hua Ping Zuo. "Relevancy between Thermochromic and Magnetic Property of La_1-xSr_xMnO₃ (x=0.2 and 0.33) Smart Radiation Thin Film Materials Prepared by Magnetron Sputtering." Applied Mechanics and Materials 303-306 (February 2013): 7–11. http://dx.doi.org/10.4028/www.scientific.net/amm.303-306.7.

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La1-xSrxMnO3 thin films with x=0.2 and 0.33 were prepared by magnetron sputtering method for its potential application on thermal control of spacecraft. The materials show a phase transition from ferromagnetic metal phase with a low infrared emittance to paramagnetic insulator phase with a high emittance. Because of the thermochromic property, they can automatically change their infrared emittance greatly in response to environment temperature and thermal load and keep the spacecraft electronic components working normally. A superconduction quantum interference device magnetometer was used to

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28

Panaitov, G., M. Bick, Y. Zhang, and H. ‐J Krause. "Peculiarities of SQUID magnetometer application in TEM." GEOPHYSICS 67, no. 3 (2002): 739–45. http://dx.doi.org/10.1190/1.1484516.

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Due to progress in high‐temperature superconductor (HTS) technology, research in the application of superconducting quantum interference devices (SQUIDs) in time‐domain transient electromagnetics (TEM) has intensified. Several TEM systems using HTS SQUIDs have been developed and tested in numerous field trials. In this paper, the reliability of SQUID TEM data is investigated by comparison with commonly used induction‐coil data. Generally, a good agreement between SQUID and coil TEM data was found. However, two effects were observed with the SQUID TEM system which were not visible in coil measu

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29

Goswami, Srijit, Emre Mulazimoglu, Ana M. R. V. L. Monteiro, et al. "Quantum interference in an interfacial superconductor." Nature Nanotechnology 11, no. 10 (2016): 861–65. http://dx.doi.org/10.1038/nnano.2016.112.

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30

de Graaf, S. E., S. T. Skacel, T. Hönigl-Decrinis, et al. "Charge quantum interference device." Nature Physics 14, no. 6 (2018): 590–94. http://dx.doi.org/10.1038/s41567-018-0097-9.

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31

Takagaki, Y., and K. H. Ploog. "Quantum interference effects in semiconductor–superconductor microjunctions." Superlattices and Microstructures 25, no. 5-6 (1999): 659–67. http://dx.doi.org/10.1006/spmi.1999.0707.

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32

Bondarenko, S. I., V. P. Koverya, A. V. Krevsun, and L. V. Gnezdilova. "Measurement of energy gaps in superconductors by means of quantum interference devices." Low Temperature Physics 41, no. 3 (2015): 179–85. http://dx.doi.org/10.1063/1.4915915.

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33

Takeuchi, Shingo. "Holographic superconducting quantum interference device." International Journal of Modern Physics A 30, no. 09 (2015): 1550040. http://dx.doi.org/10.1142/s0217751x15500402.

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We present a holographic model of the SQUID (Superconducting QUantum Interference Device) in the external magnetic field. The model of the gravitational theory considered in this paper is the Einstein–Maxwell-complex scalar model on the four-dimensional anti-de Sitter Schwarzschild black brane geometry, where one space direction is compacted into a circle and we arrange the coefficient of the time components profile so that we can model the SQUID, where the profile plays the role of the chemical potential for the Cooper pair.

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34

Nojima, Hideo. "Superconducying Quantum Interference Device Magnetometer." IEEJ Transactions on Sensors and Micromachines 117, no. 9 (1997): 437–42. http://dx.doi.org/10.1541/ieejsmas.117.437.

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35

Duvauchelle, J. E., A. Francheteau, C. Marcenat, et al. "Silicon superconducting quantum interference device." Applied Physics Letters 107, no. 7 (2015): 072601. http://dx.doi.org/10.1063/1.4928660.

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36

Fink, H. J., V. Grünfeld, and S. M. Roberts. "Variable superconducting quantum-interference device: Theory." Physical Review B 36, no. 1 (1987): 74–78. http://dx.doi.org/10.1103/physrevb.36.74.

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37

Cleuziou, J. P., W. Wernsdorfer, V. Bouchiat, T. Ondarçuhu, and M. Monthioux. "Carbon nanotube superconducting quantum interference device." Nature Nanotechnology 1, no. 1 (2006): 53–59. http://dx.doi.org/10.1038/nnano.2006.54.

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38

Hasselbach, K., D. Mailly, and J. R. Kirtley. "Micro-superconducting quantum interference device characteristics." Journal of Applied Physics 91, no. 7 (2002): 4432–37. http://dx.doi.org/10.1063/1.1448864.

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39

Seredinski, Andrew, Anne W. Draelos, Ethan G. Arnault, et al. "Quantum Hall–based superconducting interference device." Science Advances 5, no. 9 (2019): eaaw8693. http://dx.doi.org/10.1126/sciadv.aaw8693.

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We present a study of a graphene-based Josephson junction with dedicated side gates carved from the same sheet of graphene as the junction itself. These side gates are highly efficient and allow us to modulate carrier density along either edge of the junction in a wide range. In particular, in magnetic fields in the 1- to 2-T range, we are able to populate the next Landau level, resulting in Hall plateaus with conductance that differs from the bulk filling factor. When counter-propagating quantum Hall edge states are introduced along either edge, we observe a supercurrent localized along that

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40

Mandal, Soumen, Tobias Bautze, Oliver A. Williams, et al. "The Diamond Superconducting Quantum Interference Device." ACS Nano 5, no. 9 (2011): 7144–48. http://dx.doi.org/10.1021/nn2018396.

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41

Fink, H. J., V. Grünfeld, and A. López. "Quantum-interference device without Josephson junctions." Physical Review B 35, no. 1 (1987): 35–37. http://dx.doi.org/10.1103/physrevb.35.35.

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42

Gardner, Brian W., Janice C. Wynn, Per G. Björnsson, et al. "Scanning superconducting quantum interference device susceptometry." Review of Scientific Instruments 72, no. 5 (2001): 2361–64. http://dx.doi.org/10.1063/1.1364668.

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43

Lazarides, N., and G. P. Tsironis. "rf superconducting quantum interference device metamaterials." Applied Physics Letters 90, no. 16 (2007): 163501. http://dx.doi.org/10.1063/1.2722682.

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44

Pratim Sahu, Partha. "Thermooptic reconfigurable Mach Zehnder quantum interference device." Results in Physics 12 (March 2019): 1329–33. http://dx.doi.org/10.1016/j.rinp.2018.11.101.

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45

Fagaly, R. L. "Superconducting quantum interference device instruments and applications." Review of Scientific Instruments 77, no. 10 (2006): 101101. http://dx.doi.org/10.1063/1.2354545.

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46

Burlakov, A. A., V. L. Gurtovoi, A. I. Il’in, A. V. Nikulov, and V. A. Tulin. "Superconducting quantum interference device without Josephson junctions." JETP Letters 99, no. 3 (2014): 169–73. http://dx.doi.org/10.1134/s0021364014030059.

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47

Girit, Çaǧlar, V. Bouchiat, O. Naaman, et al. "Tunable Graphene dc Superconducting Quantum Interference Device." Nano Letters 9, no. 1 (2009): 198–99. http://dx.doi.org/10.1021/nl802765x.

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48

Matsuda, Naoki, Gen Uehara, Kunio Kazami, Youichi Takada, and Hisashi Kado. "Design and Fabrication of a Multi Loop Superconducting Quantum Interference Device, the Clover-Leaf Superconducting Quantum Interference Device." Japanese Journal of Applied Physics 34, Part 2, No. 1A (1995): L27—L30. http://dx.doi.org/10.1143/jjap.34.l27.

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49

Takagaki, Y., and Y. Tokura. "Transmission resonances in a semiconductor-superconductor junction quantum interference structure." Physical Review B 54, no. 9 (1996): 6587–99. http://dx.doi.org/10.1103/physrevb.54.6587.

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50

Ao, P., and X. M. Zhu. "Quantum Interference of a Single Vortex in a Mesoscopic Superconductor." Physical Review Letters 74, no. 23 (1995): 4718–21. http://dx.doi.org/10.1103/physrevlett.74.4718.

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