M
M. B. Maple
Researcher at University of California, San Diego
Publications - 960
Citations - 27507
M. B. Maple is an academic researcher from University of California, San Diego. The author has contributed to research in topics: Superconductivity & Magnetic susceptibility. The author has an hindex of 78, co-authored 953 publications receiving 26338 citations. Previous affiliations of M. B. Maple include Chiba University & Ohio State University.
Papers
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Journal ArticleDOI
Superconducting properties of LuRh4B4
TL;DR: In this paper, measurements of the magnetization M(H) of LuRh4B4 between 1.5 K and Tc(11.45 K) are reported.
Journal ArticleDOI
Anomalous surface impedance in reentrant ferromagnetic superconductors
Chen Huang,C.E. Olsen,G. Kozlowski,H. Matsumoto,Hiroomi Umezawa,F. Mancini,M. B. Maple,H. C. Hamaker,M. S. Torikachvili,J. P. Whitehead,F. E. Wang +10 more
TL;DR: In this paper, the surface impedance penetration depth Λ of ErRh4B4 and Er0.5Ho 0.5B4 was measured by employing a spectrometer operated at 9 GHz, and it was shown that surface ferromagnetism in a ferromagnetic superconductor arises from the competition between the Meissner current shielding effect and the fluctuations of localized magnetic moments.
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μSR study of spin-glass freezing in Y1−xUxPd3 and UPd4
Wenjing Wu,Amit Keren,L. P. Le,Graeme Luke,Yasutomo J. Uemura,C. L. Seaman,Y. Dalichaouch,M. B. Maple +7 more
TL;DR: In this article, the average static random internal field H int at the muon site is found to decrease very rapidly with U concentration x, indicating that the ordered static U moment rapidly disappears with decreasing U concentration around x ≅0.2.
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Non-Fermi liquid scaling in UPdxCu5−x (x = 1, 1.5)
TL;DR: In this article, the inelastic magnetic response of UPdxCu5−x (x = 1, 1.5) for temperatures from 0.3 K to 300 K and energies between 0.5 meV and 100 meV using the neutron time of flight technique was determined.
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Surface impedance of several magnetic superconductors
TL;DR: In this article, the surface impedance of magnetic superconductors is determined by the suppression of spin fluctuations in Er 05 Ho 05 Rh 4 B 4, which gives rise to an abrupt change of Z s at the reentrant superconduction critical temperature T c 2.