Qubit Spin Convention: |0> & |1> Eigenvectors?

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SUMMARY

The discussion clarifies the convention used in quantum computing for representing qubit states, specifically |0> as (1,0)^T and |1> as (0,1)^T, which correspond to the eigenvectors of the \sigma_{z} operator. It highlights that while |0> typically denotes the ground state, both spin states have equal energy in the absence of an external field. The choice of representation is primarily for signaling binary values in communication protocols, with the spin-up state conventionally representing the off bit.

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lewis198
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This is a bit embarrassing, but by convention does [itex]|0> = (1,0)^T[/itex] and
[itex]|1>=(0,1)^T[/itex], where we are in the basis of the eigenvectors of [itex]\sigma_{z}[/itex]?
 
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The notation is a bit misleading, since [itex]|0\rangle[/itex] is most commonly used to denote the ground state of a system. However, in the absence of an external field, both spin states have the same energy. The justification for using the notation is the convention that in a communications protocol, one state must be chosen to signal binary 0 vs binary 1 for the other state. There's no particular reason to choose one over the other, but indeed the spin up state is conventionally chosen to be the off bit, see http://en.wikipedia.org/wiki/Qubit#Physical_representation
 

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