A method to control the transmission of spin waves
A spin wave and waveguide technology, applied in the field of spin wave transmission control, can solve problems such as high energy consumption, low system reliability, and complex design, and achieve low power efficiency, promote compatibility, and reduce complexity.
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Embodiment 1
[0034]This embodiment reveals the change law of the exchange interaction strength of the magnetic waveguide under the action of the electric field along the normal direction of the waveguide plane through the first principle calculation.
[0035] The calculation uses a model such as image 3 As shown in (a), it is 3 layers of bcc Fe(001) atomic layers, and its vacuum layer thickness is The electric field along the c-axis direction is introduced by the dipole layer method, and the applied electric field strength ranges from -5V / nm to 5V / nm. The calculations are based on the first-principles VASP software package, and the exchange integral J is derived from the energy difference between the antiferromagnetic and ferromagnetic states.
[0036] To simplify the description, the image 3 The iron atoms in (a) are marked as 1, 2, 3 from left to right. Considering only the nearest neighbor exchange interaction, the ferromagnetic state energy E can be obtained F and the antiferrom...
Embodiment 2
[0046] This example reveals the influence of the electric field modulation exchange effect on the spin wave transmission, the corresponding change law of the spin wave number, phase velocity, and wavelength through micromagnetic simulation, and proves the feasibility of using the electric field to regulate the exchange constant to control the spin wave transmission.
[0047] The simulation is carried out using the OOMMF software package based on the LLG equation, and the calculation especially considers the effect of the electric field modulation exchange interaction:
[0048]
[0049] in is the normalized magnetization vector, M s is the saturation magnetization, α is the Gilbert attenuation factor, and γ is the Gilbert gyromagnetic ratio. is the effective field, including Heisenberg exchange field, magnetic anisotropy field, demagnetizing field and applied bias field, which can be expressed as:
[0050]
[0051] where the exchange constant is electric field depen...
Embodiment 3
[0063] The bias magnetic field is along the x direction in the plane, and the others are the same as in Embodiment 2. The results show that the dispersion relationship of the reverse body wave can be effectively adjusted by modulating the exchange interaction intensity by an external electric field, and the wave number, phase velocity, wavelength and group velocity of the spin wave can be effectively adjusted, so the external electric field can effectively control the reverse body wave transmission.
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