In QM, can the trajectory in the phase-space split?

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Discussion Overview

The discussion centers on the nature of trajectories in phase-space within quantum mechanics (QM), particularly whether they can split, drawing comparisons to classical mechanics. Participants explore concepts related to time evolution, sensitivity to initial conditions, and the implications of different formulations of quantum mechanics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions whether the assertion that "information doesn't disappear" in QM implies that trajectories in phase-space cannot split, using the example of a simple pendulum.
  • Another participant argues that in classical mechanics, small changes in initial conditions can lead to large changes in outcomes, while in QM, the time evolution of the quantum state is linear, suggesting different behavior.
  • A participant proposes that the time evolution of a quantum state depends on the Hamiltonian and asks if a Hamiltonian could be constructed to cause non-linear time evolution.
  • It is noted that the time evolution in QM is always linear, regardless of the Hamiltonian, and distinctions are made between the Schrödinger picture and the Dirac (or interaction) picture regarding time dependence of operators and states.
  • Further links to literature are provided discussing quantum systems and their sensitivity to initial conditions, including references to Bohmian mechanics, where particles have trajectories.
  • A participant expresses interest in the complexity of the question and acknowledges the challenge in finding answers related to quantum chaos.
  • Another participant introduces a scenario involving a quadripartite system and questions the encoding of information under unitary evolution, raising further inquiries about local information and its recovery.

Areas of Agreement / Disagreement

Participants express differing views on the implications of linear time evolution in QM and its relationship to classical mechanics. There is no consensus on whether trajectories can split or how information is encoded and recovered in quantum systems.

Contextual Notes

Participants reference various formulations of quantum mechanics and the implications of Hamiltonians, but the discussion remains open-ended regarding the specifics of these relationships and the nature of information in quantum states.

Who May Find This Useful

This discussion may be of interest to those studying quantum mechanics, particularly in relation to phase-space dynamics, quantum chaos, and the foundational principles of information in quantum systems.

ORF
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Hello.

I was told that "in QM the information doesn't disappear". Does it mean that, in QM, the trajectory in the phase-space can't split? [The typical example is a vertical simple pendulum, with the mass above the spin-point; in classical mechanics you can't know if the pendulum will fall one side or another.]

If this question is already answered in this forum, just tell me, and I will delete this thread.

Thank you for your time :)

Greetings
PS: My mother language is not English, so I'll be glad if you correct any mistake.
 
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In the classical case you bring up, a small change in initial condition leads to a large change in final condition.

In the quantum case, I believe this cannot happen, because the time evolution of the quantum state is linear. This only refers to the time evolution of the state between measurements, and not to measurement outcomes, which are random and whose probabilities are given by the Born rule. However, a quick google brings up this interesting discussion:

http://arxiv.org/abs/quant-ph/9802047
http://dx.doi.org/10.1103/PhysRevA.45.R555
Quantum state sensitivity to initial conditions
Gonzalo Garcia de Polavieja
(Submitted on 17 Feb 1998)
The different time-dependent distances of two arbitrarily close quantum or classical-statistical states to a third fixed state are shown to imply an experimentally relevant notion of state sensitivity to initial conditions. A quantitative classification scheme of quantum states by their sensitivity and instability in state space is given that reduces to the one performed by classical-mechanical Lyapunov exponents in the classical limit.
 
Last edited:
Hello

Thank you for your interest (I have not access to the Physical Review A; I looked for similar papers, but with no results). Well, I suppose the time evolution of the state will depend on the Hamiltonian that you consider :)

Let's going to remake the question: can we build a Hamiltonian which cause a no-linear time evolution?

Greetings.
 
There are two links - I think the arXiv link should be free?

The time evolution (between measurements) in quantum mechanics is always linear, no matter what the Hamiltonian is.
 
Yes, the arXiv link is free, thank you for it :)

atyy said:
The time evolution (between measurements) in quantum mechanics is always linear, no matter what the Hamiltonian is.
Ouch, such a lapse of memory. Thank you, you are right: in the "Schrödinger picture", the operators are constant, and the states evolve.

But in the "Dirac picture" (or "interaction picture"), operators and states have a time dependence :)

Thank you for your interest.

Greetings
 
I found some more discussions about the relationship between quantum systems and classical systems that are sensitively dependent on the initial condition.

http://arxiv.org/abs/math-ph/0503032v2
Quantum Chaos: Spectral Analysis of Floquet Operators
James Matthew McCaw

http://xxx.lanl.gov/abs/quant-ph/9906092
Continuous Quantum Measurement and the Emergence of Classical Chaos
Tanmoy Bhattacharya, Salman Habib, Kurt Jacobs

The thesis by James McCaw has an interesting overview of the literature. One things he mentions is that in the Bohmian formulation, particles do have trajectories, so one can ask whether Bohmian particles exhibit sensitive dependence on their initial conditions.
 
Hello

I only gave the McCaw's work a glance, but it looks a very good starting point (I didn't know anything about quantum chaos when I did the question).

The question seemed to me simple, but finding an answer is harder than I thought :)

Thank you for the links, I am going to read them right now.

Greetings!
 
ORF said:
I was told that "in QM the information doesn't disappear".

I am interested too.
Let us take a quadripartite system. It is in an initial pure state say 0110>
each particle has a complete local information. There is an unitary evolution operator U(t) which act on the state. Local information may disappear. But ## U^{-1}## will give it back
where is encoded the information at time t?
 

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