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Entanglement

There is a fundamental difference between the \bgroup\color{col1}$ M=\pm 1$\egroup states \bgroup\color{col1}$ \vert T_{\pm 1}\rangle$\egroup on the one side and the \bgroup\color{col1}$ M=0$\egroup states \bgroup\color{col1}$ \vert S\rangle$\egroup and \bgroup\color{col1}$ \vert T_0\rangle$\egroup on the other side: For product states of two particles 1 and 2 (pure tensors),
$\displaystyle \vert\psi\rangle_1 \otimes \vert\phi\rangle_2,$     (2.15)

one can say that particle 1 is in state \bgroup\color{col1}$ \vert\psi\rangle$\egroup and particle 2 is in state \bgroup\color{col1}$ \vert\phi\rangle$\egroup. States that can not be written as product states are called entangled states. For example, for the state
$\displaystyle \vert\psi\rangle_1 \otimes \vert\phi\rangle_2 + \vert\phi\rangle_1 \otimes \vert\psi\rangle_2,$     (2.16)

one can not say which particle is in which state: the two particles are entangled. Entanglement is the key concept underlying all modern quantum information theory, such as quantum cryptography, quantum teleportation, or quantum computing.


next up previous contents index
Next: The Exchange Interaction Up: Properties of Spin-Singlets and Previous: Total Spin   Contents   Index
Tobias Brandes 2005-04-26