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Chapter 5: Architecture - Computer and Information Science - CUNY

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5.1. BITS AND QUBITS 3<br />

A bit is either in state |0〉 or in state |1〉, which was sufficient for the classical<br />

world. Either electricity is running through a circuit or it is not. Either a switch<br />

is on or it is off. Either a proposition is true or it is false. But either/or is not<br />

sufficient in the quantum world. In that world, there are situations where we<br />

are in one state <strong>and</strong> in the other simultaneously. In the realm of the quantum<br />

world, there are systems where a switch is both on <strong>and</strong> off. One quantum<br />

system can be in state |0〉 <strong>and</strong> in state |1〉. Hence we are led to the definition<br />

of a qubit:<br />

Definition 5.1.1 A quantum bit or a qubit is a way of describing a quantum<br />

system of dimension two.<br />

We shall represent a qubit as a two by one matrix with complex numbers<br />

[ ]<br />

0 c 0<br />

, (5.3)<br />

1 c 1<br />

where |c 0 | 2 + |c 1 | 2 = 1. Notice that a classical bit is a special type of qubit.<br />

|c 0 | 2 is to be interpreted as the probability that after measuring the qubit, it<br />

will be found in state |0〉. |c 1 | 2 is to be interpreted as the probability that<br />

after measuring the qubit it will be found in state |1〉. Whenever we measure a<br />

qubit, it automatically becomes a bit. So we shall never “see” a general qubit.<br />

Nevertheless, they do exist <strong>and</strong> are the main characters in our tale. We might<br />

visualize this “collapsing” of a qubit to a bit as<br />

<br />

[1, 0] T<br />

[c 0 , c 1 ] T<br />

[0, 1]. T (5.4)<br />

Following the normalization procedures that we learned in chapter 4 on page<br />

???, any element of C 2 can be converted into a qubit. For example, the vector<br />

⎡ ⎤<br />

V = ⎣ 5 + 3i ⎦ (5.5)<br />

6i

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