Dynamics at Solid State Surfaces and Interfaces. In contrast, the decrease in the resistance at about 85 Oe occurred very quickly, due to the magnetization reversal in the thicker NiFe layer. In bulky magnetic materials, the effect of such anisotropy is negligible, because the volume fraction of the interface parts is very small. The author initially focused his research on fine particles. Nanomagnetism and Spintronics by.
|Date Added:||18 February 2007|
|File Size:||25.80 Mb|
|Operating Systems:||Windows NT/2000/XP/2003/2003/7/8/10 MacOS 10/X|
|Price:||Free* [*Free Regsitration Required]|
We are unable to offer combined shipping for multiple items purchased. Principles of Radiation Interaction in Matter and Detection.
Nanomagnetism and Spintronics – Google Books
When the thickness was 0. No trivia or quizzes yet. Analysis of autochthonous lactic acid bacteria from mozzarella cheese production. The spectrum for the top interface is fairly broad and the average hyperfine field is smaller than the bulk Fe value.
The Mg layer thickness was 1. In other words, MR measurements can be used to verify that the sign of interlayer coupling is negative.
If the sample included a significant amount of Mg impurities, the amorphous structure would be stable and the transformation to a bcc structure spintronnics not take place.
Overall rating No ratings yet 0. Colloidal Quantum Nanomagentism Optoelectronics and Photovoltaics. Although the MR ratio of the spin-valve system is not large, satisfactorily high magnetoresistance sensitivity was achieved. Biophysical Chemistry of Biointerfaces. However, the prepared samples were frozen immediately after preparation to protect their surface from chemical reaction and therefore the measurement temperature had to be much lower nanomagnwtism room temperature.
Sincehe has been a specially-appointed professor at Osaka University and a senior researcher at the International Institute for Advanced Studies. No, cancel Yes, report it Thanks! The major driving force is attributed to the spin-torque of the electric current flowing in the ferromagnetic wire.
Nanomagnetism and Spintronics Teruya Shinjo. In comparison with the field-driven case, current driven magnetization reversal is advantageous also to enhance the density of magnetic memories.
Nevertheless, current driven domain wall motion is an spinttronics research area for further development of spintronics. Nanomagnetism and Spintronics by. Seth marked it as to-read Nov 07, The main target for most of them was the creation of new superconducting materials.
There was a problem providing the content you requested
The spectrum for the 0. In general, the vacuum condition before the s was not high enough to produce reliable samples. The displacement of the domain wall was found to proceed very quickly. These materials are regarded as new materials that do not exist in nature. The concise and accessible chapters of Nanomagnetism and Spintronics, Second Edition, cover the most recent research in areas of spin-current generation, spin-calorimetric effect, voltage effects on magnetic properties, spin-injection phenomena, giant magnetoresistance GMRand tunnel magnetoresistance TMR.
Sep 22, goei. Quantum Cylinders of Graphene. Moreover, in the area of magnetism research, multilayers were regarded as one of the most interesting subjects.
B 43— [ PubMed ]. Several other groups as well were preparing and investigating multilayers and many new laboratories designed for their study were opening up. This result, indicating that there are two crystallographic sites having different nanomagnetism and spintronics by teruya shinjo moments, was important to the understanding of the magnetic properties of this compound.
However, the amorphous form of pure Fe is known to be unstable. Introduction to Graphene-Based Nanomaterials.