Science, Том 319,Выпуски 5859-5864John Michels (Journalist) American Association for the Advancement of Science, 2008 |
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... Field -0.3 -0.2 -0.1 0 0.1 Fig . 1. ( A. R Si 16. S. Mashchenko , H. M. P. Couchman , J. Wadsley , Nature 442 , 539 ... field opposite to the expectations within the Abrikosov - Ginzburg - Landau paradigm . We propose that the anomalous ...
... Field -0.3 -0.2 -0.1 0 0.1 Fig . 1. ( A. R Si 16. S. Mashchenko , H. M. P. Couchman , J. Wadsley , Nature 442 , 539 ... field opposite to the expectations within the Abrikosov - Ginzburg - Landau paradigm . We propose that the anomalous ...
Стр. 178
... field ( clockwise starting in the top left corner ) . Images at the two lowest fields [ ( A ) and ( B ) ] are based on earlier mea- surements ( 17 ) . The orientation of the crystal lattice is shown in ( A ) . ( D to F ) Schematics of ...
... field ( clockwise starting in the top left corner ) . Images at the two lowest fields [ ( A ) and ( B ) ] are based on earlier mea- surements ( 17 ) . The orientation of the crystal lattice is shown in ( A ) . ( D to F ) Schematics of ...
Стр. 179
... field de- pendence shown by the dashed lines . Below 2 TF2 is essentially constant , in agreement with Fig . 2. Structural phase diagram for the VL in CeColn , with the magnetic field parallel to the c axis . The exact location of the ...
... field de- pendence shown by the dashed lines . Below 2 TF2 is essentially constant , in agreement with Fig . 2. Structural phase diagram for the VL in CeColn , with the magnetic field parallel to the c axis . The exact location of the ...
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