They say superposition enables qubit to live in linear superposition of two states. I.e. \begin{equation} |\phi\rangle = a|0\rangle + b |1\rangle \end{equation}
Why are we interested only in linear combination of the two states ?
They say superposition enables qubit to live in linear superposition of two states. I.e. \begin{equation} |\phi\rangle = a|0\rangle + b |1\rangle \end{equation}
Why are we interested only in linear combination of the two states ?
A qubit is defined as living in a 2-dimensional Hilbert space. This means one cannot define more than 2 linearly independent basis states. Since $|0\rangle$ and $|1\rangle$ are linearly independent (they are actually orthogonal), any other state must be in their span, so written as a linear combination $a|0\rangle+b|1\rangle$. This is a fact from linear algebra, not from quantum mechanics. (Mixed states are a bit more general, but same idea of 2 linearly independent basis states.)
Now of course one can define another quantum system that lives in an $n$-dimensional Hilbert space! Then we will talk about linear combinations of $n$ different basis states, like $a|0\rangle+b|1\rangle+\cdots + z|n-1\rangle$. These are still interesting for quantum mechanics! It just so happens that most quantum computational algorithms start with qubits as their basic ingredients, in analogy with bits for classical computation, but there is no physical reason to be restricted to such. In fact, one can even talk about infinite dimensional Hilbert spaces; people do this all the time.