Spin squeezing is a quantum process that decreases the variance of one of the angular momentum quadratures below the standard quantum limit, at the expense of increasing variance in another, in an ensemble of particles with spin. This is achieved by somehow entangling the individual spin states within the ensemble.The quantum states obtained are called spin squeezed states. Such states have been proposed for quantum metrology, to allow a better precision for estimating a rotation angle than classical interferometers.
Mathematical definition Spin squeezed states for an ensemble of spins have been defined analogously to squeezed states of a bosonic mode. Spin squeezed states are often defined with reference to an ensemble of spin-1/2 particles. These particles have 3 quadratures ( J x , J y , J z ) {\displaystyle (J_{x},J_{y},J_{z})} along which spin can be measured. Each of these quadratures has eigenvalues ± 1 2 {\displaystyle \pm {\frac {1}{2}}} . The way that uncertainty manifests itself in this quantum system derives from the commutation relations between these different spin operators:
[ J i , J j ] = i ϵ i j k J k {\displaystyle [J_{i},J_{j}]=i\epsilon _{ijk}J_{k}}
where ϵ i j k {\displaystyle \epsilon _{ijk}} is the Levi-Cevita symbol. Therefore, by the Heisenberg uncertainty relation, ( Δ J x ) 2 ( Δ J y ) 2 ⩾ 1 4 | ⟨ J z ⟩ | 2 {\displaystyle (\Delta J_{x})^{2}(\Delta J_{y})^{2}\geqslant {\frac {1}{4}}|\langle J_{z}\rangle |^{2}}
For an ensemble of spins, the J i {\displaystyle J_{i}} are the collective angular momentum components defined as J i = ∑ n j i ( n ) , {\displaystyle J_{i}=\sum _{n}j_{i}^{(n)},} where j i ( n ) {\displaystyle j_{i}^{(n)}} are the single particle angular momentum components. We say that the state is spin-squeezed in the x {\displaystyle x} -direction, if the variance of the x {\displaystyle x} -component is smaller than the square root of the right-hand side of the inequality above ( Δ J x ) < 1 2 | ⟨ J z ⟩ | . {\displaystyle (\Delta J_{x})<{\frac {1}{2}}|\langle J_{z}\rangle |.} A different definition was based on using states with a reduced spin-variance for metrology.
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