Zobrazeno 1 - 10
of 1 727
pro vyhledávání: '"C W, Schneider"'
Publikováno v:
Applied Physics. A, Materials Science & Processing
LixLaySrzMnO3 thin films of various compositions (x,y,z) have been grown using pulsed laser deposition. The compositions of the films have been studied as a function of deposition temperature, target-to-substrate distance and deposition pressure with
Publikováno v:
Physical Review Materials
Autor:
Irvine, Thomas1,2 (AUTHOR) tirv41@hawaii.edu, Wysor, Brian2 (AUTHOR) tirv41@hawaii.edu, Beauvais, Alicia2 (AUTHOR)
Publikováno v:
Diversity (14242818). Sep2024, Vol. 16 Issue 9, p554. 42p.
Publikováno v:
Algae. Sep2024, Vol. 39 Issue 3, p149-161. 13p.
Autor:
Schneider, Craig W.1 cschneid@trincoll.edu, Cianciola, Elisabeth N.1, Popolizio, Thea R.2, Spagnuolo, Dylan S.1, Lane, Christopher E.2
Publikováno v:
Algae. Mar2015, Vol. 30 Issue 1, p15-33. 19p.
Autor:
Liu Y; UNSW Materials and Manufacturing Futures Institute, School of Materials Science and Engineering, The University of New South Wales, Kensington, NSW, 2052, Australia., Meng Q; UNSW Materials and Manufacturing Futures Institute, School of Materials Science and Engineering, The University of New South Wales, Kensington, NSW, 2052, Australia., Mahmoudi P; UNSW Materials and Manufacturing Futures Institute, School of Materials Science and Engineering, The University of New South Wales, Kensington, NSW, 2052, Australia., Wang Z; UNSW Materials and Manufacturing Futures Institute, School of Materials Science and Engineering, The University of New South Wales, Kensington, NSW, 2052, Australia., Zhang J; UNSW Materials and Manufacturing Futures Institute, School of Materials Science and Engineering, The University of New South Wales, Kensington, NSW, 2052, Australia., Yang J; UNSW Materials and Manufacturing Futures Institute, School of Materials Science and Engineering, The University of New South Wales, Kensington, NSW, 2052, Australia., Li W; UNSW Materials and Manufacturing Futures Institute, School of Materials Science and Engineering, The University of New South Wales, Kensington, NSW, 2052, Australia., Wang D; UNSW Materials and Manufacturing Futures Institute, School of Materials Science and Engineering, The University of New South Wales, Kensington, NSW, 2052, Australia., Li Z; UNSW Materials and Manufacturing Futures Institute, School of Materials Science and Engineering, The University of New South Wales, Kensington, NSW, 2052, Australia., Sorrell CC; UNSW Materials and Manufacturing Futures Institute, School of Materials Science and Engineering, The University of New South Wales, Kensington, NSW, 2052, Australia., Li S; UNSW Materials and Manufacturing Futures Institute, School of Materials Science and Engineering, The University of New South Wales, Kensington, NSW, 2052, Australia.
Publikováno v:
Advanced materials (Deerfield Beach, Fla.) [Adv Mater] 2024 Oct; Vol. 36 (42), pp. e2405009. Date of Electronic Publication: 2024 Aug 06.
Autor:
S. Das, K. Sen, I. Marozau, M. A. Uribe-Laverde, N. Biskup, M. Varela, Y Khaydukov, O. Soltwedel, T. Keller, M. Dobelli, C. W. Schneider, C. Bernhard
Publikováno v:
Physical Review B.
Publikováno v:
Physica C: Superconductivity. 328:53-59
We have measured the thermal conductivity κ of Bi2(SrCa)3(Cu1−xTx)2Oy (T=Ni,Co,Fe) whiskers containing up to 1.5% substitution for Cu. Increased substitution suppresses both Tc and the usual enhancement of κ seen below Tc in undoped samples. Addi
Autor:
C. W. Schneider, D. T. Verebelyi, J. M. Pond, He Li, M. V. Nevitt, M. J. Skove, G. X. Tessema, Y. K. Kuo
Publikováno v:
Physica C: Superconductivity. 319:1-11
We have grown single crystal whiskers of Bi 2 (SrCa) n +1 (Cu 1− x Co x ) n O 8− δ with 0 x R as a function of the temperature T . For x n =2 in the majority of the sample and n =3 in a small part. For both phases, the changes in T c and in the
Publikováno v:
Physical Review B. 56:6201-6206
We have measured the change in the resistive ${T}_{c}$ of ${\mathrm{Bi}}_{2}(\mathrm{SrCa}{)}_{2+n}({\mathrm{Cu}}_{1\ensuremath{-}x}{M}_{x}{)}_{1+n}{\mathrm{O}}_{y}$ whiskers due to substitution of $M$ = Ni (magnetic) or $M$ = Zn (nonmagnetic) for Cu