Quantum Theory Flashcards
Quantum Theory
What are the De Broglie relations and when do they apply (D)
E=hw (Energy, constant, angular frequency)
p=hk (Momentum vector, constant, wave vector)
They apply for a free particle (no forces / V=0)
Quantum Theory
What is the Schrodinger equation? (D)
ih * βπΉ/βt = - h^2 / 2m * β^2πΉ + VπΉ
Quantum Theory
What is the stationary state Schrodinger equation? (D)
- h^2 / 2m * β^2π+Vπ=Eπ
Quantum Theory
How do you arrive at the stationary state equation from the Schrodinger equation? (Q)
You look for separable solutions. Let πΉ(x,t)=π(x)T(t) and divide by it to get:
( ih dT/dt ) / T
= ( - h^2 / 2m * β^2π + Vπ ) / π
= constant
= E
Quantum Theory
What is the one-dimensional Schrodinger equation? (D)
ih * βπΉ/βt = - h^2 / 2m * β^2πΉ/dx^2 + VπΉ
Quantum Theory
What is the one-dimensional stationary state Schrodinger equation? (D)
- h^2 / 2m * d^2π/dx^2 + Vπ = Eπ
Quantum Theory
What are the stationary state solutions and associated energies of the one-dimensional particle in a box? (Q)
πn(x)=Bsin(npix/a)
Energy: En=n^2 pi^2 h^2 / 2ma^2
Quantum Theory
What are the wave functions of the one-dimensional particle in a box? (Q)
πΉn(x,t)=Bsin(npix/a) * e^( -i n^2 pi^2 h t / 2 m a^2 )
Quantum Theory
What is the ground state energy? (D)
When the possible energies of a quantum system are discrete and bounded below, the ground state energy is the smallest energy state
Quantum Theory
What are the stationary state solutions and associated energies of the three-dimensional particle in a box? (Q)
πn1,n2,n3(x,y,z)= Bsin(n1pix/a)sin(n2piy/b)sin(n3piz/c)
With energies En1,n2,n3
= pi^2 h^2 / 2m ( n1^2/a^2 + n2^2/b^2 + n3^2/c^2 )
Quantum Theory
What does it mean to say an energy level E has d-fold degeneracy? (D)
It means the space of solutions to the stationary state schrodinger equation with energy level E has a dimension d>1. When d=1 we call E a non-degenerate energy state
Quantum Theory
What is the correspondence principle? (D)
The tendency for quantum results to tend to the classical result as the quantum number tends to β (as the energy of the system increases)
Quantum Theory
What is the probability density function for the particles position? (D)
The square of the magnitude of the wave function
Quantum Theory
What does it mean for a wave function to be normalised? (D)
For the integral over all space of the magnitude square of the wave function to be equal to 1
Quantum Theory
What does it mean for a wave function to be normalisable? (D)
For the integral over all space of the magnitude square of the wave function to be strictly between 0 and β
Quantum Theory
What is the continuity equation? (D)
βΟ/βt + βΒ·j = 0
Quantum Theory
What is the probability current j? (D)
j(X,t) = ih / 2m ( πΉ*conj(βπΉ)-conj(πΉ)βπΉ )
Quantum Theory
Whatβs the rough proof of the continuity equation? (T)
Note Β¦πΉ(x,t)Β¦^2 = conj(πΉ)πΉ.
Differentiate with product rule
Expand with Schrodinger
Then collect terms and note β^2 = βΒ·β
Quantum Theory
What is the condition for int[R^3] Β¦πΉΒ¦^2 dxdydz to be independent of t? (T)
j must tend to 0 faster than 1/Β¦xΒ¦^2 as Β¦xΒ¦ ->β
Quantum Theory
Prove the theorem that if j tends to 0 faster than 1/Β¦xΒ¦^2 as Β¦xΒ¦ -> β. Then the integral of R^3 of Β¦πΉΒ¦^2 is independent of time. (T)
Idea of proof if to look at the derivative of the integral of a general space D with border S. Use continuity. Divergence. Then transform to spherical. Let S be sphere and show it tends to 0 as r->β.
Proof in Chapter 3 notes
Quantum Theory
3 conditions on solutions to the Schrodinger equation? (Q)
The wave function should be a continuous, single valued function. This means the probability density is single-valued with no discontinuities
The wave function should be normalisable
βπΉ should be continuous everywhere, except when there is an infinite discontinuity in V. This follows as discontinuity in βπΉ => infinite discontinuity in β^2πΉ => infinite discontinuity in V from Schrodinger
Quantum Theory
When solving an IVP for a particle in a box, how to you calculate the coefficients cn? (Q)
[0]int[a] f(x)πm(x) dx = [n=1]sum[β] ( cn * [0]int[a] πn(x)πm(x) dx ) = cm
Since [0]int[a] πmπn dx = 0 as they are orthogonal
The 2nd equality comes from the fourier series for f(x)
Quantum Theory
What is the probability of measuring the energy of the particle to be En? (Q)
¦cn¦^2
Quantum Theory
Show [n=1]sum[β] Β¦cnΒ¦^2 = 1 (T)
1
= [0]int[a] Β¦πΉΒ¦^2 dx
= [m,n=1]sum[β] of conj(cm)cn * e^-i(En-Em)t/h * [0]int[a] conj(πm)πn dx
= [n=1]sum[β] Β¦cnΒ¦^2
2nd equality from series expansion of πΉ. 3rd equality since π is real