The principle of deferred measurement plays a important role in understanding the interaction between a quantum computer and its environment. In the field of quantum information, this principle allows us to delay the measurement of a quantum system until a later point in time, enabling more complex computational operations and preserving the delicate quantum coherence.
In a quantum computer, information is stored in quantum bits, or qubits, which can exist in superposition states. These superpositions enable quantum computers to perform parallel computations and potentially solve certain problems more efficiently than classical computers. However, qubits are extremely sensitive to their environment, which can cause decoherence and lead to the loss of quantum information.
The interaction between a quantum computer and its environment can be described using the framework of quantum mechanics. According to this framework, any measurement performed on a quantum system causes it to collapse into one of its possible states. This collapse is known as the "measurement postulate" and is a fundamental aspect of quantum theory.
Deferred measurement allows us to postpone the collapse of a quantum system by delaying the measurement operation. This means that we can perform additional quantum operations on the qubits before extracting the final measurement result. By deferring the measurement, we can manipulate the quantum state of the system and perform complex computations.
To illustrate the principle of deferred measurement, let's consider an example involving two qubits in a superposition state. Suppose we have qubit A in a superposition of states |0⟩ and |1⟩, and qubit B in a superposition of states |+⟩ and |−⟩. The joint state of the two qubits can be written as:
|Ψ⟩ = α|0⟩⨂|+⟩ + β|0⟩⨂|−⟩ + γ|1⟩⨂|+⟩ + δ|1⟩⨂|−⟩,
where α, β, γ, and δ are complex probability amplitudes.
If we were to measure qubit A immediately, the state of the system would collapse to one of the four possible outcomes: |0⟩⨂|+⟩, |0⟩⨂|−⟩, |1⟩⨂|+⟩, or |1⟩⨂|−⟩. However, by deferring the measurement of qubit A, we can perform additional quantum operations on qubit B before making the measurement.
For instance, we could apply a quantum gate to qubit B that rotates its state around the Bloch sphere. This gate operation would affect the superposition amplitudes β and δ, modifying the final measurement probabilities. Only after performing these additional operations, we would measure qubit A and extract the final measurement result.
Deferred measurement is particularly valuable in quantum error correction and fault-tolerant quantum computation. By delaying the measurement, we can implement error correction codes that detect and correct errors without collapsing the quantum state prematurely. This allows quantum computers to perform reliable computations even in the presence of noise and decoherence.
The principle of deferred measurement is a fundamental concept in quantum information. It enables the manipulation of quantum states without prematurely collapsing them, allowing for more complex computations and preserving quantum coherence. By deferring the measurement of a quantum system, we can perform additional quantum operations and implement error correction codes, enhancing the robustness and reliability of quantum computation.
Other recent questions and answers regarding Classical control:
- Does the basis with vectors called |+> and |-> represent a maximally non-orthogonal basis in relation to the computational basis with vectors called |0> and |1> (meaning that |+> and |-> are at 45 degrees in relation to 0> and | 1>)?
- Why is classical control important for implementing quantum computers and performing quantum operations?
- How does the width of a Gaussian distribution in the field used for classical control affect the probability of distinguishing between emission and absorption scenarios?
- Why is the process of flipping the spin of a system not considered a measurement?
- What is classical control in the context of manipulating spin in quantum information?

