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Pseudomagnetic fields

To continue, we assume the following situation We concentrate on an x-y plane, which is chosen to be perpendicular to the seam. In this way, the pseudomagnetic field is guaranteed to be perpendicular to the plane and will have a nonzero component in the z direction only. In addition, we locate the origin at the point of the singularity, that is, at the crossing point between the plane and the seam. With these definitions the pseudomagnetic field is assumed to be of the form [113]. [Pg.690]

Dirac 8 function, non-adiabatic coupling, curl condition, pseudomagnetic field,... [Pg.74]


See other pages where Pseudomagnetic fields is mentioned: [Pg.635]    [Pg.639]    [Pg.688]    [Pg.689]    [Pg.690]    [Pg.692]    [Pg.768]    [Pg.60]    [Pg.73]    [Pg.80]    [Pg.88]    [Pg.94]    [Pg.94]    [Pg.100]    [Pg.766]    [Pg.770]    [Pg.819]    [Pg.820]    [Pg.821]    [Pg.823]    [Pg.441]    [Pg.442]    [Pg.468]    [Pg.40]    [Pg.44]    [Pg.93]    [Pg.94]    [Pg.95]    [Pg.97]    [Pg.816]   


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Curl condition pseudomagnetic field

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