The spectral theorem is a fundamental concept in quantum mechanics that relates to the properties of observables. It provides a mathematical framework for understanding the spectrum of possible values that can be observed when measuring a physical quantity. In this answer, we will explore the spectral theorem in detail and discuss its significance in relation to observables.
The spectral theorem states that for a self-adjoint operator on a Hilbert space, there exists a unique decomposition of the operator into a sum of projection operators. These projection operators correspond to the eigenstates of the operator, and the eigenvalues associated with these states represent the possible outcomes of measurements of the observable.
To understand the significance of the spectral theorem, let's consider an example. Suppose we have a quantum system with a self-adjoint operator representing the observable of energy. The spectral theorem tells us that this operator can be decomposed into a sum of projection operators, each associated with a specific energy eigenstate. The eigenvalues of the operator correspond to the possible energy values that can be observed when measuring the system.
This decomposition allows us to determine the probability of measuring a specific energy value. The probability is given by the square of the projection of the state vector onto the corresponding eigenstate. By measuring the energy of the system multiple times and collecting statistics, we can verify the predictions of the spectral theorem.
The spectral theorem also provides a basis for understanding the completeness and orthogonality of the eigenstates. These properties are important for the formulation of quantum mechanics and the calculation of probabilities. Furthermore, the spectral theorem allows us to express observables as a sum of operators acting on the eigenstates, which simplifies calculations and provides a clear physical interpretation.
The spectral theorem is a fundamental concept in quantum mechanics that relates to the properties of observables. It provides a mathematical framework for understanding the spectrum of possible values that can be observed when measuring a physical quantity. The theorem allows us to decompose observables into a sum of projection operators associated with eigenstates, providing a basis for calculating probabilities and simplifying calculations.
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

