Quantum system time evolution

In summary, a quantum system with a Hamiltonian H and normalised eigenstates ψn has a linear operator Q defined by its action on these states. Q has eigenvalues 1 and -1 and corresponding normalised eigenstates ζ1 and ζ2, which are expressed in terms of energy eigenstates. The expectation value of H is calculated to be (E1 + E2)/2 for both states ζ1 and ζ2. When a measurement of Q is made at time=0 and the result 1 is obtained, the system then evolves according to the Schrodinger equation. The probability that the result will again be 1 if a measurement is made at a time T = pi*h/(E2
  • #1
mcheung4
22
0

Homework Statement



A quantum system has Hamiltonian H with normalised eigenstates ψn and corresponding energies En (n = 1,2,3...). A linear operator Q is defined by its action on these states:

1 = ψ2
2 = ψ1
n = 0, n>2

Show that Q has eigenvalues 1 and -1 and find the corresponding normalised eigenstates ζ1 and ζ2, in terms of energy eigenstates. Calculate <H> in each of the states ζ1 and ζ2.

A measurement of Q is made at time=0, and the result 1 is obtained. The system is then left undisturbed for a time t, at which instant another measurement of Q is made. What is the probability that the result will again be 1? Show that the probability is 0 if the measurement is made after a time T = [itex]\pi[/itex]ħ/(E2 - E1), assuming E2 - E1> 0.

Homework Equations





The Attempt at a Solution



I found
ζ1 = (ψ1 + ψ2)/√2
ζ2 = (ψ1 - ψ2)/√2
and <H> = (E1 + E2)/2 for both.

I have trouble doing the second part.

Doesnt the system collapse into ζ1 given we know this is the state at time =0?
so probability will be 1?
 
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  • #2
The wave function collapses to [itex] \zeta_1 [/itex] after measurement but after that, it will evolve by Schrodinger equation and so it will change gradually. You should apply the time evolution operator to the state [itex] \zeta_1[/itex] and then calculate the inner product of the evolved state with [itex] \zeta_1 [/itex].
 
  • #3
Shyan said:
The wave function collapses to [itex] \zeta_1 [/itex] after measurement but after that, it will evolve by Schrodinger equation and so it will change gradually. You should apply the time evolution operator to the state [itex] \zeta_1[/itex] and then calculate the inner product of the evolved state with [itex] \zeta_1 [/itex].

so ψ(x,0) = (ψ1 + ψ2)/√2,
and U(t,0) = exp(-iHt/ħ),
then ψ(x,t) = U(t,0)ψ(x,0) = exp(-iHt/ħ)(ψ1 + ψ2)/√2

inner product :
∫ [exp(iHt/ħ)((ψ1)* + (ψ2)*)/√2][(ψ1 + ψ2)/√2] dx
= exp(iHt/ħ)

is this correct? but i don't know what H is here, is it (E1+E2)/2?
 
  • #4
mcheung4 said:
so ψ(x,0) = (ψ1 + ψ2)/√2,
and U(t,0) = exp(-iHt/ħ),
then ψ(x,t) = U(t,0)ψ(x,0) = exp(-iHt/ħ)(ψ1 + ψ2)/√2

inner product :
∫ [exp(iHt/ħ)((ψ1)* + (ψ2)*)/√2][(ψ1 + ψ2)/√2] dx
= exp(iHt/ħ)

is this correct? but i don't know what H is here, is it (E1+E2)/2?

The point you're missing, is how to act on [itex] \psi [/itex]s by the evolution operator.
[itex]
e^{\frac{iHt}{\hbar}}\psi_n=\sum_{m=0}^{\infty} (\frac{iH_nt}{\hbar})^m \frac{ \psi_n}{m!}=\sum_{m=0}^{\infty} (\frac{it}{\hbar})^m \frac{H^m \psi_n}{m!}=\sum_{m=0}^{\infty} (\frac{it}{\hbar})^m \frac{E_n^m \psi_n}{m!}=\sum_{m=0}^{\infty} (\frac{iE_nt}{\hbar})^m \frac{ \psi_n}{m!}=e^{\frac{iE_n t}{\hbar}}\psi_n
[/itex]

So you don't need to know H!
 
  • #5
so ψ(0) = (ψ1 + ψ2)/√2, ψ(t) = U(t,0)ψ(0) = exp(-iHt/ħ)(ψ1 + ψ2)/√2 = [exp(-iE1t/ħ)ψ1 + exp(-iE2t/ħ)ψ]/√2. then find the probability amplitude of (ψ1 + ψ2)/√2 in this time-varying state by taking the inner product ((ψ1 + ψ2)/√2 , ψ(t)), squared it to find the probability = [1 + cos((E2-E1)t/h)]/2, then sub in T = pi*h/(E2-E1) indeed got probability = 0. but why after T it'll stay 0? doesn't it cycle again by the consine term?
 
  • #6
mcheung4 said:
so ψ(0) = (ψ1 + ψ2)/√2, ψ(t) = U(t,0)ψ(0) = exp(-iHt/ħ)(ψ1 + ψ2)/√2 = [exp(-iE1t/ħ)ψ1 + exp(-iE2t/ħ)ψ]/√2. then find the probability amplitude of (ψ1 + ψ2)/√2 in this time-varying state by taking the inner product ((ψ1 + ψ2)/√2 , ψ(t)), squared it to find the probability = [1 + cos((E2-E1)t/h)]/2, then sub in T = pi*h/(E2-E1) indeed got probability = 0. but why after T it'll stay 0? doesn't it cycle again by the consine term?

Why do you say it remains zero? Just because it becomes 0 momentarily does not mean it stays at 0.
 
  • #7
mcheung4 said:
so ψ(0) = (ψ1 + ψ2)/√2, ψ(t) = U(t,0)ψ(0) = exp(-iHt/ħ)(ψ1 + ψ2)/√2 = [exp(-iE1t/ħ)ψ1 + exp(-iE2t/ħ)ψ]/√2. then find the probability amplitude of (ψ1 + ψ2)/√2 in this time-varying state by taking the inner product ((ψ1 + ψ2)/√2 , ψ(t)), squared it to find the probability = [1 + cos((E2-E1)t/h)]/2, then sub in T = pi*h/(E2-E1) indeed got probability = 0. but why after T it'll stay 0? doesn't it cycle again by the consine term?
I think you simply misread the question but I can see how the phrasing may lead to confusion. What they meant is that at the time T = pi*h/(E2-E1) after the initial measurement was made the probability is zero, but they do not mean to say that it will remain zero for all times after that instant. They really just meant at that specific instant, not at all later times. So you are right, it will cycle again.
 
  • #8
ok thanks guys!
 

1. What is quantum system time evolution?

Quantum system time evolution refers to the way in which a quantum system changes and evolves over time, according to the laws of quantum mechanics. This evolution can be described using mathematical equations, such as the Schrödinger equation, which take into account factors such as the system's initial state and the Hamiltonian operator.

2. How does quantum system time evolution differ from classical system time evolution?

Quantum system time evolution differs from classical system time evolution in several ways. In classical mechanics, the state of a system can be precisely determined at any given time and can be predicted with certainty. However, in quantum mechanics, the state of a system is described by a wave function that can only give probabilities for different outcomes. Additionally, quantum systems can exist in a state of superposition, where they can simultaneously occupy multiple states, while classical systems can only exist in one state at a time.

3. What factors influence the time evolution of a quantum system?

The time evolution of a quantum system is influenced by several factors, including the system's initial state, the Hamiltonian operator, and any external forces or interactions. The Hamiltonian operator takes into account the system's energy and potential, and how they change over time. External forces, such as electromagnetic fields, can also affect the time evolution of a quantum system.

4. Can the time evolution of a quantum system be controlled or manipulated?

Yes, the time evolution of a quantum system can be controlled and manipulated through techniques such as quantum measurement and quantum control. By measuring the system at different times, it is possible to gain information about its state and change its evolution. Quantum control involves using external forces to manipulate the Hamiltonian and alter the system's time evolution.

5. What applications does understanding quantum system time evolution have?

Understanding quantum system time evolution is crucial for various applications in fields such as quantum computing, quantum information processing, and quantum simulations. By understanding and controlling the time evolution of quantum systems, it is possible to design and develop new technologies that utilize the unique properties of quantum mechanics, such as superposition and entanglement.

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