The particle in a box model is a simplified quantum mechanical system that allows us to study the behavior of a particle confined within a one-dimensional box. In this model, the particle is assumed to be free to move within the box, but it cannot escape its boundaries.
To find the energy eigenvalues and eigenstates of the particle in a box, we start by solving the time-independent Schrödinger equation for this system. The Schrödinger equation describes the behavior of quantum systems and is given by:
Hψ = Eψ
Here, H is the Hamiltonian operator, ψ is the wave function, E is the energy eigenvalue, and ℏ is the reduced Planck's constant.
For the particle in a box, the Hamiltonian operator can be written as:
H = -((ℏ^2)/(2m)) * d^2/dx^2
where m is the mass of the particle and d^2/dx^2 represents the second derivative with respect to position.
To solve the Schrödinger equation, we assume that the wave function ψ can be written as a product of a spatial part and a time part:
ψ(x, t) = Ψ(x) * exp(-iEt/ℏ)
where Ψ(x) represents the spatial part of the wave function and exp(-iEt/ℏ) represents the time part.
Substituting this expression into the Schrödinger equation and separating the variables, we obtain:
-(ℏ^2)/(2m) * d^2Ψ/dx^2 = EΨ
This is a second-order linear differential equation that can be solved by assuming a form for Ψ(x) that satisfies the boundary conditions of the particle in a box. The boundary conditions are that the wave function must be zero at the boundaries of the box.
For a particle in a box of length L, the boundary conditions give rise to standing wave solutions, where the wave function is zero at the boundaries and has a specific number of nodes within the box. The number of nodes is determined by the quantum number n, which can take on integer values (n = 1, 2, 3, …).
The spatial part of the wave function for the particle in a box is given by:
Ψ(x) = √(2/L) * sin(nπx/L)
where n is the quantum number and x is the position within the box.
The energy eigenvalues for the particle in a box are given by:
E = (n^2π^2ℏ^2)/(2mL^2)
where n is the quantum number, m is the mass of the particle, ℏ is the reduced Planck's constant, and L is the length of the box.
The relationship between the wave vector and the energy eigenvalues can be understood by considering the de Broglie wavelength of the particle. According to the de Broglie hypothesis, particles can exhibit wave-like behavior, and their wavelength is related to their momentum.
The wave vector k is defined as:
k = (2π)/λ
where λ is the wavelength of the particle.
For the particle in a box, the wavelength of the particle is related to the length of the box and the quantum number n:
λ = 2L/n
Substituting this expression into the definition of the wave vector, we get:
k = (2π)/(2L/n) = (nπ)/L
The energy eigenvalues can be written in terms of the wave vector as:
E = (k^2ℏ^2)/(2m)
Substituting the expression for k, we obtain:
E = ((nπ)^2ℏ^2)/(2mL^2)
which is consistent with the energy eigenvalues derived earlier.
The process of finding the energy eigenvalues and eigenstates of the particle in a box involves solving the time-independent Schrödinger equation for the system and applying the appropriate boundary conditions. The energy eigenvalues are determined by the quantum number n, which corresponds to the number of nodes in the wave function. The relationship between the wave vector and the energy eigenvalues arises from the de Broglie wavelength of the particle.
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

