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Phys 825 Homework 1: Electric Charge, Vector Potential, and Complex Field Lagrangians, Assignments of Quantum Physics

The first homework assignment for a university-level physics course, focusing on electric charge, vector potential, and complex field lagrangians. Students are asked to demonstrate the dimensionless nature of electric charge in a specific unit system, find the charge of an electron, derive maxwell's equations from the vector potential lagrangian, and identify the equation of motion for a complex field lagrangian.

Typology: Assignments

2019/2020

Uploaded on 09/22/2020

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Phys 825
homework #1
due Thurs. Sept. 3
1. In SI units the permittivity of free space is 0= 8.85 ×1012 C2/N·m2. In this
course it will be convenient to set 0= 1. This defines our unit of charge.
(i) Show that in ¯h=c=0= 1 units electric charge is dimensionless.
(ii) In these units, what is the charge of an electron?
2. Consider the following Lagrangian for the vector potential Aµ,
L=1
4Fµν Fµν
where Fµν =µAννAµis the field strength.1
Vary the corresponding action with respect to Aµ. Show that the principle of
least action gives the two Maxwell equations which aren’t already implied by
writing the field strength in terms of the vector potential.
3. Consider the following Lagrangian for a complex field ψ(t, x).
L=i¯ψ
∂t ¯h2
2m~
ψ·~
ψV(x)ψψ
What is the equation of motion? Does it look familiar? We’ll have more to say
about this Lagrangian later in the course.
Hint: when you have a complex field, you can vary ψand ψas though they
were independent fields. If you don’t believe this, set ψ=ψ1+2and show
that varying the real and imaginary parts separately leads to the same answer.
1I’m setting c=0=µ0= 1. If you want to restore units I think it should be L=1
4µ0FµνFµν .

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Phys 825 homework # due Thurs. Sept. 3

  1. In SI units the permittivity of free space is  0 = 8. 85 × 10 −^12 C^2 /N · m^2. In this course it will be convenient to set  0 = 1. This defines our unit of charge.

(i) Show that in ¯h = c =  0 = 1 units electric charge is dimensionless. (ii) In these units, what is the charge of an electron?

  1. Consider the following Lagrangian for the vector potential Aμ,

L = −

Fμν F μν

where Fμν = ∂μAν − ∂ν Aμ is the field strength.^1 Vary the corresponding action with respect to Aμ. Show that the principle of least action gives the two Maxwell equations which aren’t already implied by writing the field strength in terms of the vector potential.

  1. Consider the following Lagrangian for a complex field ψ(t, x).

L = i¯hψ∗^

∂ψ ∂t

¯h^2 2 m

∇~ψ∗^ · ∇~ψ − V (x)ψ∗ψ

What is the equation of motion? Does it look familiar? We’ll have more to say about this Lagrangian later in the course. Hint: when you have a complex field, you can vary ψ and ψ∗^ as though they were independent fields. If you don’t believe this, set ψ = ψ 1 + iψ 2 and show that varying the real and imaginary parts separately leads to the same answer.

(^1) I’m setting c =  0 = μ 0 = 1. If you want to restore units I think it should be L = − (^41) μ 0 Fμν^ F^

μν (^).