Difference between revisions of "Spin Orbit Coupling"

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===Square lattice===
 
===Square lattice===
 
The experimental realization is published here <ref>PRL 121, 150401 (2018)</ref>. 2 orthogonal beams are sent back and forth to create a square lattice:
 
The experimental realization is published here <ref>PRL 121, 150401 (2018)</ref>. 2 orthogonal beams are sent back and forth to create a square lattice:
<math>V_{latt}=V_0\cos^2(k_0 x)+V_0\sin^2(k_0 y)</math>. The total Hamiltonian of the system reads as <math>\hat H = \frac{p^2}{2m}+V_{latt}+\Omega_{R}(x,y)+\frac{\delta}{2}\sigma_z</math>
+
<math>V_{latt}=V_0\cos^2(k_0 x)+V_0\sin^2(k_0 y)</math>. The total Hamiltonian of the system reads as <math>\hat H = \frac{p^2}{2m}+V_{latt}+\Omega_{R}(x,y)+\frac{\delta}{2}\sigma_z</math>, where δ is the two-photon detuning. By tuning the phase between two beams δφ it is possible to transition from 1D to 2D SOC. For phases δφ=0, π, they demonsrate 1D SOC. For phases δφ=±π/2 they have symmetrical 2D SOC.
<ref> </ref>
+
<ref> </ref>.
 
<math></math>
 
<math></math>
 +
 
==References==
 
==References==
 
[[Category:BEC]]
 
[[Category:BEC]]

Revision as of 14:06, 3 February 2020

Creation of 2D SOC

Square lattice

The experimental realization is published here [1]. 2 orthogonal beams are sent back and forth to create a square lattice: V_{latt}=V_0\cos^2(k_0 x)+V_0\sin^2(k_0 y). The total Hamiltonian of the system reads as \hat H = \frac{p^2}{2m}+V_{latt}+\Omega_{R}(x,y)+\frac{\delta}{2}\sigma_z, where δ is the two-photon detuning. By tuning the phase between two beams δφ it is possible to transition from 1D to 2D SOC. For phases δφ=0, π, they demonsrate 1D SOC. For phases δφ=±π/2 they have symmetrical 2D SOC. [2].


References

  1. PRL 121, 150401 (2018)