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<math>p = \frac{1}{1 + cos2\eta}</math> | <math>p = \frac{1}{1 + cos2\eta}</math> | ||
== | ==Pseudocode== | ||
The probabilistic cloning machine can only perform effectively for a special set of input states. It was shown that states chosen from a set <math>S = \{|\psi_1\rangle, |\psi_2\rangle, ..., |\psi_n\rangle,\}</math> can be probabilistic-ally cloned if and only if the <math>|\psi_i\rangle</math> are linearly independent. This protocol in general consists of three stages as follows: | The probabilistic cloning machine can only perform effectively for a special set of input states. It was shown that states chosen from a set <math>S = \{|\psi_1\rangle, |\psi_2\rangle, ..., |\psi_n\rangle,\}</math> can be probabilistic-ally cloned if and only if the <math>|\psi_i\rangle</math> are linearly independent. This protocol in general consists of three stages as follows: | ||
===General case=== | ===General case=== |