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  2. Magnetic 2D materials - Wikipedia

    en.wikipedia.org/wiki/Magnetic_2D_materials

    Magnetic 2D materials can be used as a part of van der Waals heterostructures. They are layered materials consisting of different 2D materials held together by van der Waals forces. One example of such structure is a thin insulating/semiconducting layer between layers of 2D magnetic material, producing a magnetic tunnel junction.

  3. File:Slow moving vehicle.svg - Wikipedia

    en.wikipedia.org/wiki/File:Slow_moving_vehicle.svg

    Although it is free of copyright restrictions, this image may still be subject to other restrictions. See WP:PD § Fonts and typefaces or Template talk:PD-textlogo for more information. This image is too simple to be copyrighted, and is a public sign required to be used for various purposes.

  4. File:Block magnet.svg - Wikipedia

    en.wikipedia.org/wiki/File:Block_magnet.svg

    You are free: to share – to copy, distribute and transmit the work; to remix – to adapt the work; Under the following conditions: attribution – You must give appropriate credit, provide a link to the license, and indicate if changes were made. You may do so in any reasonable manner, but not in any way that suggests the licensor endorses ...

  5. Van Vleck paramagnetism - Wikipedia

    en.wikipedia.org/wiki/Van_Vleck_paramagnetism

    The Hamiltonian for an electron in a static homogeneous magnetic field in an atom is usually composed of three terms = + (+) + where is the vacuum permeability, is the Bohr magneton, is the g-factor, is the elementary charge, is the electron mass, is the orbital angular momentum operator, the spin and is the component of the position operator orthogonal to the magnetic field.

  6. Magnetic flux - Wikipedia

    en.wikipedia.org/wiki/Magnetic_flux

    If the magnetic field is constant, the magnetic flux passing through a surface of vector area S is = = ⁡, where B is the magnitude of the magnetic field (the magnetic flux density) having the unit of Wb/m 2 , S is the area of the surface, and θ is the angle between the magnetic field lines and the normal (perpendicular) to S.

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