In Quantum States and Probabilities, we saw that a quantum state can be expressed as a combination of the and states as follows:
The parameters and are the amplitudes whose squares are the probabilities of collapsing to 0 or 1, respectively.
We can express the quantum state more compactly. Since a qubit is a blended state of just the two quantum states, and , we can represent it as a vector of two rows and one column (see Working with Matrices and Vectors):
In this vector, the top element represents the amplitude for the pentagon qubelets, and the bottom represents the amplitude for the triangle qubelets in the qubit.
The vector for the idealized quantum state will have and :
Pictorially, this vector represents the following qubelets in the qubit:
The triangle qubelet is drawn with a dotted outline as it’s not active in this qubit.
Likewise, the vector for the idealized quantum state will have and :
In this case, this vector corresponds to the following qubelets in the qubitshown.
The pentagon qubelet is drawn with a dotted outline since it’s not active in the qubit.
Consider a qubit with seven pentagon qubelets and three inverted triangle qubelets, shown in the following figure:
You can calculate its quantum state as described in Quantum States and Probabilities to get:
Rewrite this equation as a vector:
Sometimes, you’ll find it convenient to write the previous vector in terms of the vectors for the idealized quantum states and , as shown here:
In general, the quantum state of a single qubit in terms of vectors is:
The squares of the amplitudes and still add up to 1 for the vector to be a valid representation of a quantum state:
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