LayMuon
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I am reading about spontaneous symmtry breaking for superconductors and came a cross to this simple statement:
Here is the potential for complex scalar field: V = 1/2 \lambda^2 (|\phi|^2 -\eta^2)^2.
Scalar field is small and we can expand its modulus around \eta:
<br /> <br /> \phi(x) = |\phi(x)| e^{i \alpha(x)} = (\eta + \frac{1}{\sqrt{2}} \phi(x)) e^{i \alpha(x)}<br />
How did he do that expansion?
Here is the potential for complex scalar field: V = 1/2 \lambda^2 (|\phi|^2 -\eta^2)^2.
Scalar field is small and we can expand its modulus around \eta:
<br /> <br /> \phi(x) = |\phi(x)| e^{i \alpha(x)} = (\eta + \frac{1}{\sqrt{2}} \phi(x)) e^{i \alpha(x)}<br />
How did he do that expansion?