Multilayer film heterostructure, its preparation method and application
A heterogeneous structure and multi-layer film technology, which is applied to devices that apply electro-magnetic effects, thermoelectric devices that only use Peltier or Seebeck effects, instruments, etc., can solve the limitation of coercive force film thickness and the mixing of spin Seebeck effect , unfavorable spin current detection and other problems, to increase the number and expand the range of materials
- Summary
- Abstract
- Description
- Claims
- Application Information
AI Technical Summary
Problems solved by technology
Method used
Image
Examples
Embodiment 1
[0052] This example is used to illustrate the preparation method of the multilayer film heterostructure provided by the present invention.
[0053] The sample was grown on a GGG substrate (3mm×5mm×0.5mm) with 13 μm YIG(Y 3 Fe 5 o 12 ) film, in which YIG is a ferrimagnetic insulator, and then Cu (3nm), CoPt (5nm), IrMn (8nm), SiO 2 (5nm), among which Cu, CoPt, IrMn adopt DC sputtering method, SiO 2 The radio frequency sputtering method adopted, the vacuum degree of the magnetron sputtering equipment is less than 4.0×10 -5 Pa, the working pressure of argon is 0.5Pa.
[0054] The prepared sample GGG / YIG / Cu(3nm) / CoPt(5nm) / IrMn(8nm) / SiO 2 (5nm) is a multilayer heterogeneous structure, such as figure 2 shown.
Embodiment 2-11
[0056] This embodiment is used to illustrate the measurement effect of the longitudinal spin Seebeck effect measurement device provided by the present invention.
[0057] Adopt the preparation method described in embodiment 1 to prepare described sample, all embodiments all adopt GGG substrate (3mm * 5mm * 0.5mm), wherein the material and thickness of each layer are as follows:
[0058]
[0059] The hysteresis loop of embodiment 2 sample GGG / YIG is as Figure 4 shown. The hysteresis loop shows that YIG is an in-plane film and isotropic in the plane. The hysteresis loop of the sample GGG / YIG is measured by a vibrating sample magnetometer, and the in-plane saturation field is about 30Oe.
Embodiment 3
[0060] Example 3 Sample GGG / Cu(3nm) / CoPt(5nm) / IrMn(8nm) / SiO 2 (5nm) hysteresis loop such as Figure 5 shown. Since Cu has a long spin diffusion length and weak spin-orbit coupling, it is an ideal isolation layer to eliminate the ferromagnetic exchange coupling between the ferromagnetic layers YIG and CoPt. Measurement of sample GGG / Cu(3nm) / CoPt(5nm) / IrMn(8nm) / SiO with a vibrating sample magnetometer 2 The hysteresis loop (5nm) shows that the bias field obviously deviates from the zero field, and the left and right coercive forces are far outside the saturation field of the GGG / YIG sample.
PUM
Property | Measurement | Unit |
---|---|---|
thickness | aaaaa | aaaaa |
thickness | aaaaa | aaaaa |
Abstract
Description
Claims
Application Information
- R&D Engineer
- R&D Manager
- IP Professional
- Industry Leading Data Capabilities
- Powerful AI technology
- Patent DNA Extraction
Browse by: Latest US Patents, China's latest patents, Technical Efficacy Thesaurus, Application Domain, Technology Topic, Popular Technical Reports.
© 2024 PatSnap. All rights reserved.Legal|Privacy policy|Modern Slavery Act Transparency Statement|Sitemap|About US| Contact US: help@patsnap.com