- #1
LayMuon
- 149
- 1
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: [itex] V = 1/2 \lambda^2 (|\phi|^2 -\eta^2)^2 [/itex].
Scalar field is small and we can expand its modulus around [itex] \eta [/itex]:
[tex]
\phi(x) = |\phi(x)| e^{i \alpha(x)} = (\eta + \frac{1}{\sqrt{2}} \phi(x)) e^{i \alpha(x)}
[/tex]
How did he do that expansion?
Here is the potential for complex scalar field: [itex] V = 1/2 \lambda^2 (|\phi|^2 -\eta^2)^2 [/itex].
Scalar field is small and we can expand its modulus around [itex] \eta [/itex]:
[tex]
\phi(x) = |\phi(x)| e^{i \alpha(x)} = (\eta + \frac{1}{\sqrt{2}} \phi(x)) e^{i \alpha(x)}
[/tex]
How did he do that expansion?