stranhuz
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Dear forum people,
I just learned how to get a tight-binding dispersion for graphene:
E = +- \sqrt{1+4\cos((\sqrt{3}a/2) k_x)\cos((a/2) k_y)+4\cos^2((a/2) k_y)}
But i can not figure out how can I plot that. I want to plot that in the following path: K \rightarrow \Gamma \rightarrow M \rightarrow K.
I think k_y = 0 in the line \Gamma M and I should plot(E,k_x); k_x = constant in the line MK and I should plot(E,k_y); but I don't know how the plot() is look like for K \Gamma, where both k_x and k_y are not constant.
For nanotube, I was able to do that becouse we just had k, so I just made "plot(E,k,'b')". Here in graphene, we have both k_x, k_y.
I would be appreciated if could some one give me a hand on my problem.
Best wishes for all.
I just learned how to get a tight-binding dispersion for graphene:
E = +- \sqrt{1+4\cos((\sqrt{3}a/2) k_x)\cos((a/2) k_y)+4\cos^2((a/2) k_y)}
But i can not figure out how can I plot that. I want to plot that in the following path: K \rightarrow \Gamma \rightarrow M \rightarrow K.
I think k_y = 0 in the line \Gamma M and I should plot(E,k_x); k_x = constant in the line MK and I should plot(E,k_y); but I don't know how the plot() is look like for K \Gamma, where both k_x and k_y are not constant.
For nanotube, I was able to do that becouse we just had k, so I just made "plot(E,k,'b')". Here in graphene, we have both k_x, k_y.
I would be appreciated if could some one give me a hand on my problem.
Best wishes for all.