kof9595995
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Let's say a two electron state for Helium atom, I've seen author (Sakurai, Modern QM,section 6.4) wrote \Phi ({x_1},{x_2})\chi as the most general form, where \Phi ({x_1},{x_2}) is either a symmetric or antisymmetric wave function, and \chi is the singlet or triplet state respectively. But how about this kinda state:
{\psi _a}({x_1}){\psi _b}({x_2})| \uparrow \downarrow > - {\psi _a}({x_2}){\psi _b}({x_1})| \downarrow \uparrow >
It's also antisymmetric, so isn't it also a possible state?
{\psi _a}({x_1}){\psi _b}({x_2})| \uparrow \downarrow > - {\psi _a}({x_2}){\psi _b}({x_1})| \downarrow \uparrow >
It's also antisymmetric, so isn't it also a possible state?