In the field of Quantum Information, specifically in the study of Quantum Entanglement in systems of two qubits, the probability of observing a specific state can be related to the magnitudes squared of the corresponding complex numbers through the principles of quantum mechanics. To understand this relationship, it is important to first grasp the concept of a qubit and the mathematical representation of its states.
A qubit is the fundamental unit of quantum information, analogous to a classical bit. However, unlike a classical bit that can only be in either a 0 or 1 state, a qubit can exist in a superposition of both states simultaneously. Mathematically, a qubit is represented as a linear combination of the basis states |0⟩ and |1⟩, where the coefficients of the linear combination are complex numbers. For example, a general state of a single qubit can be written as:
|ψ⟩ = α|0⟩ + β|1⟩
Here, α and β are complex numbers that represent the probability amplitudes of the qubit being in state |0⟩ and |1⟩, respectively. The probability of observing the qubit in a specific state is given by the magnitude squared of the corresponding complex number. In this case, the probability of observing the qubit in state |0⟩ is |α|^2, and the probability of observing it in state |1⟩ is |β|^2.
Now, let's consider a system of two qubits. The state of this system can be described by a tensor product of the individual qubit states. For example, if we have qubit A in state |ψ_A⟩ and qubit B in state |ψ_B⟩, the combined state of the two qubits is given by:
|ψ⟩ = |ψ_A⟩ ⊗ |ψ_B⟩
In this case, the probability of observing a specific state of the two-qubit system depends on the magnitudes squared of the corresponding complex numbers associated with that state. Let's consider an example to illustrate this.
Suppose we have two qubits, qubit A and qubit B. Qubit A is in the state |0⟩, which can be represented as:
|0⟩ = 1|0⟩ + 0|1⟩
Qubit B is in the state |1⟩, which can be represented as:
|1⟩ = 0|0⟩ + 1|1⟩
The combined state of the two qubits is then:
|ψ⟩ = |0⟩ ⊗ |1⟩ = (1|0⟩ + 0|1⟩) ⊗ (0|0⟩ + 1|1⟩)
Expanding this expression, we get:
|ψ⟩ = 1|0⟩⊗|0⟩ + 0|0⟩⊗|1⟩ + 0|1⟩⊗|0⟩ + 1|1⟩⊗|1⟩
Simplifying further, we obtain:
|ψ⟩ = |01⟩
In this case, the probability of observing the two-qubit system in the state |01⟩ is |1|^2 = 1. The probabilities of observing the system in other states, such as |00⟩, |10⟩, or |11⟩, can be calculated similarly.
In a two-qubit system, the probability of observing a specific state is related to the magnitudes squared of the corresponding complex numbers associated with that state. This relationship arises from the principles of quantum mechanics and the mathematical representation of qubits. By calculating the magnitudes squared, we can determine the likelihood of observing a particular state in a given two-qubit system.
Other recent questions and answers regarding EITC/QI/QIF Quantum Information Fundamentals:
- Are amplitudes of quantum states always real numbers?
- How the quantum negation gate (quantum NOT or Pauli-X gate) operates?
- Why is the Hadamard gate self-reversible?
- If measure the 1st qubit of the Bell state in a certain basis and then measure the 2nd qubit in a basis rotated by a certain angle theta, the probability that you will obtain projection to the corresponding vector is equal to the square of sine of theta?
- How many bits of classical information would be required to describe the state of an arbitrary qubit superposition?
- How many dimensions has a space of 3 qubits?
- Will the measurement of a qubit destroy its quantum superposition?
- Can quantum gates have more inputs than outputs similarily as classical gates?
- Does the universal family of quantum gates include the CNOT gate and the Hadamard gate?
- What is a double-slit experiment?
View more questions and answers in EITC/QI/QIF Quantum Information Fundamentals

