Students review using the Arms representation to represent states for discrete quantum systems and connecting the Arms representation to histogram and matrix representation. The student then extend the Arms representation to begin exploring the continuous position basis.
1. << Dimensional Analysis of Kets | Completeness Relations |
2. << Time Evolution of a Quantum Particle on a Ring with Arms | Arms Sequence for Complex Numbers and Quantum States |
This activity is part of the Arms Sequence for Complex Numbers and Quantum States.
Students should be familiar with spin-1/2 and spin-1 systems, particularly represently quantum states with Dirac notation, histograms, matrices, and arms.
Set-Up
Instructor writes a quantum state in Dirac notation on the board. “How would you represent this state using arms?”
The instructor then asks the pair of volunteers (volunteers should write their answer on the board):
Instructor asks.“What would we have to do in order to represent a spin-1 state with arms?” Answer - add a student.
Instructor repeats exercise for a spin-3 system (7 basis kets)
Instructor asks the students to consider a new situation: “Now imagine that I have a particle and the position of the particle in an observable I'm interested in.”
“How could we present a quantum state in the position basis with Arms?” Ask as many students as volunteer to join the Arms representation. Still not enough - we'd need an infinite number of people! And an infinite number of people in between each person.
What would the histogram look like? Answer: A function of x. This is the wavefunction.
What would a quantum state written in a 1-D position basis look like? Answer: An infinitely long column with each entry corresponding a position eigenstate. The set of all the entries is the wavefunction.
in Dirac notation, label with the eigenvalue:
\[\hat{X}\left|{x}\right\rangle =x\left|{x}\right\rangle \]
Complete - can write down a completion relation. The sum for a discrete basis, like spin, become an integral for a continuous basis:
\[ \sum_{s} \left|{s}\right\rangle \left\langle {s}\right| = 1 \]
\[ \int \left|{x}\right\rangle \left\langle {x}\right| dx = 1 \]
Talk about the dimensions of \(\left|{x}\right\rangle \rightarrow\) 1/\(\sqrt{\mbox{length}}\)
Write a state in the position basis by applying a completeness relation:
\begin{align*} \left|{\psi}\right\rangle &= \left(\int \left|{x}\right\rangle \left\langle {x}\right| dx \right) \left|{psi}\right\rangle \\ &= \int \left|{x}\right\rangle \left\langle {x}\middle|{\psi}\right\rangle dx \\ &= \int \left\langle {x}\middle|{\psi}\right\rangle \left|{x}\right\rangle dx \\ &= \int \psi(x) \left|{x}\right\rangle dx \\ \end{align*}
Notice: \(\left\langle {x}\middle|{\psi}\right\rangle \) is the wavefunction. Because of the integral, we can't just take the norm squared of the wavefunction at a particular x to get the probability of the particle being at a particular location. The wavefunction doesn't have the right dimensions! Instead, the wavefunction is a “probability amplitude density”. If you square the wavefunction, you get a probability density. You have to integrate the norm square of the wavefunction over a length to get a probability.
In fact, asking the question “What is the probability of the particle being at a particular point?” is not a question we can answer with the formalism of quantum mechanics. We can only calculate the probability of a particle being in an infinitesimal region:
\[\mathcal{P}(\mbox{between }x_0 \mbox{ and }x_0+dx) = |\left\langle {x}\middle|{\psi}\right\rangle |^2 dx\]
The multiplication by \(dx\) makes the quantity dimensionless.
To calculate the probability of the particle being in a finite region:
\[\mathcal{P}(\mbox{between }x=a \mbox{ and }x=b) = \int_a^b |\left\langle {x}\middle|{\psi}\right\rangle |^2 dx\]