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I have just started to study quantum mechanics, so I have some doubts.
1) if I consider the base given by the eigenstates of s_z s_z | \pm >=\pm \frac{\hbar}{2} |\pm> the spin operators are represented by the matrices
s_x= \frac {\hbar}{2} (|+><-|+|-><+|)
s_y= i \frac {\hbar}{2}(|-><+|-|+><-|)
s_z=\frac{\hbar}{2}(|+><+|-|-><-|)
but I don't have clear idea of what they correspond to concretely. Considering the Dirac formalism, can they be represented by Pauli's matrices?
s_x=\frac {\hbar}{2} \sigma_x; s_y= i \frac {\hbar}{2} \sigma_y; s_z=\frac {\hbar}{2} \sigma_z
2) I can write a vector using its components, e.g. v=(a,b)
but which are the components of the eigenstates of s_z?
3) If I have a state such as s_x |\phi>=\frac {\hbar}{2} |\phi>
and I want to write it using the base of the eigenstates of s_z,
can I write |\phi>=a|+>+b|->, with |a|^2+|b|^2=1? (I need this condition to have a normalized vector)
Is it equal to \frac {e^{i\theta}}{\sqrt 2}(|+>+|->)?
Many thanks for your help!
1) if I consider the base given by the eigenstates of s_z s_z | \pm >=\pm \frac{\hbar}{2} |\pm> the spin operators are represented by the matrices
s_x= \frac {\hbar}{2} (|+><-|+|-><+|)
s_y= i \frac {\hbar}{2}(|-><+|-|+><-|)
s_z=\frac{\hbar}{2}(|+><+|-|-><-|)
but I don't have clear idea of what they correspond to concretely. Considering the Dirac formalism, can they be represented by Pauli's matrices?
s_x=\frac {\hbar}{2} \sigma_x; s_y= i \frac {\hbar}{2} \sigma_y; s_z=\frac {\hbar}{2} \sigma_z
2) I can write a vector using its components, e.g. v=(a,b)
but which are the components of the eigenstates of s_z?
3) If I have a state such as s_x |\phi>=\frac {\hbar}{2} |\phi>
and I want to write it using the base of the eigenstates of s_z,
can I write |\phi>=a|+>+b|->, with |a|^2+|b|^2=1? (I need this condition to have a normalized vector)
Is it equal to \frac {e^{i\theta}}{\sqrt 2}(|+>+|->)?
Many thanks for your help!