Quantum mechanics formalisms and conservation of energy

In summary, quantum mechanics formalisms describe the behavior of particles at the quantum level, utilizing mathematical constructs such as wave functions and operators. These formalisms uphold the principle of conservation of energy, indicating that the total energy of a closed system remains constant over time. Quantum systems can exchange energy through interactions, but the overall energy remains conserved, aligning with classical mechanics while introducing unique phenomena like superposition and entanglement.
  • #1
KleinMoretti
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5
TL;DR Summary
conservation of energy after measurement in different formalism of qm
in a recent thread @PeterDonis said that in standard quantum mechanics a system being measured must be considered open and you need to include the measurement device if you want to talk about conservation of energy, my question is if the formalism of qm used changes anything here?
 
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  • #2
KleinMoretti said:
the formalism of qm used
What do you mean by this?
 
  • #3
PeterDonis said:
What do you mean by this?
so for example if you used the Heisenberg picture as oppose to the Schrödinger
 
  • #4
KleinMoretti said:
so for example if you used the Heisenberg picture as oppose to the Schrödinger
Why would that make a difference? Both pictures are mathematically equivalent and make the same predictions.
 
  • #5
so what you said in that thread I mentioned,
"However, it should be noted that, in basic QM (i.e., without adopting any particular interpretation--discussion of how particular QM interpretations deal with collapse belongs in the interpretations subforum), "collapse" is not claimed to be an actual physical process; it's just an update you make in your mathematical model when you know the result of a measurement. Since making a measurement on a quantum system requires the system to be open, i.e., it has to interact with other systems, one would not expect conservation laws to hold for the measured system alone, since conserved quantities can be exchanged through the interaction. For example, the measured system could gain or lose energy from the interaction that takes place during meaurement, so its energy taken in isolation would not be conserved. Only the energy of the whole larger system, including the measuring device and anything else the measuring device interacted with, would be conserved."

is true regardless of the picture of qm you use right?
 
  • #6
KleinMoretti said:
is true regardless of the picture of qm you use right?
It's true in both the Heisenberg and Schrodinger pictures, yes.
 
  • #7
PeterDonis said:
It's true in both the Heisenberg and Schrodinger pictures, yes.
so just for further clarification when someone says something is true or holds in standard or basic qm, the formulation (e.g Heisenberg, Schrödinger, interaction, etc) is not relevant?
 
  • #8
KleinMoretti said:
when someone says something is true or holds in standard or basic qm, the formulation (e.g Heisenberg, Schrödinger, interaction, etc) is not relevant?
Yes.
 
  • #9
PeterDonis said:
Yes.
The reason I asked is because I came across a thread in physics stack that mentions that there are ways to make the Heisenberg and Schrödinger formulations non-equivalent and then I remember your comment from that previous thread here and got me wondering if the formulation one uses changes anything regarding conservation of energy after measurement.
 
  • #10
KleinMoretti said:
I came across a thread in physics stack that mentions that there are ways to make the Heisenberg and Schrödinger formulations non-equivalent
Two of the papers referenced in that response are talking about quantum field theory, which is different from non-relativistic QM. In QFT it's not even clear at the outset what the "pictures" mean, since their definition requires a notion of "time evolution" (the difference in "pictures" in NRQM is in how much of the time evolution you put in the states vs. the operators), and in QFT there is no such notion, at least not in the basic formulation, because any such notion would be frame-dependent.

The other paper talks about methods of quantization other than the Born-Jordan prescription. That paper appears to be talking about NRQM, but AFAIK nobody actually uses any other methods in NQRM. I don't think that paper's analysis would even apply to QFT, since in QFT the whole question of "methods of quantization" is different.
 
  • #11
PeterDonis said:
Two of the papers referenced in that response are talking about quantum field theory, which is different from non-relativistic QM. In QFT it's not even clear at the outset what the "pictures" mean, since their definition requires a notion of "time evolution" (the difference in "pictures" in NRQM is in how much of the time evolution you put in the states vs. the operators), and in QFT there is no such notion, at least not in the basic formulation, because any such notion would be frame-dependent.

The other paper talks about methods of quantization other than the Born-Jordan prescription. That paper appears to be talking about NRQM, but AFAIK nobody actually uses any other methods in NQRM. I don't think that paper's analysis would even apply to QFT, since in QFT the whole question of "methods of quantization" is different.
another reason I was curious is because whenever I look through discussions or questions regarding QM (for example my question about conservation of energy in QM in that previous thread) most answers are with respect to quantum mechanics in general without mention of a formulation/picture which is why I wonder if that simply meant the answer is true regardless of the formulation/picture.
 
  • #12
KleinMoretti said:
I wonder if that simply meant the answer is true regardless of the formulation/picture.
As has been stated, it does.

At this point the OP question has been answered and this thread is closed.
 

FAQ: Quantum mechanics formalisms and conservation of energy

What is the relationship between quantum mechanics and the conservation of energy?

In quantum mechanics, the conservation of energy is a fundamental principle that states that the total energy of an isolated system remains constant over time. This principle is upheld in quantum systems, where energy levels of particles are quantized. Transitions between these energy levels occur through interactions, but the total energy before and after the interaction remains the same.

How does the concept of energy quantization relate to conservation of energy?

Energy quantization in quantum mechanics means that particles can only possess specific energy levels. While these levels are discrete, transitions between them involve the absorption or emission of energy in the form of photons. Even though energy is exchanged during these transitions, the overall conservation of energy is maintained, as the energy before and after the process remains equal.

Can energy conservation be violated in quantum mechanics?

In quantum mechanics, energy conservation is not violated, but it may appear so in certain scenarios, such as in virtual particles or during quantum fluctuations. These phenomena occur within the limits set by the uncertainty principle, which allows for temporary violations of energy conservation on very short timescales. However, when considering the entire system over a longer period, energy conservation holds true.

How is the conservation of energy expressed mathematically in quantum mechanics?

The conservation of energy in quantum mechanics is often expressed through the time-dependent Schrödinger equation, which describes how the quantum state of a system evolves over time. The Hamiltonian operator, which represents the total energy of the system, plays a crucial role in this equation. When the Hamiltonian is time-independent, it leads to the conservation of energy, as the expectation value of the energy remains constant during the evolution of the system.

What role do symmetries play in the conservation of energy in quantum mechanics?

In quantum mechanics, symmetries play a vital role in the conservation laws, including the conservation of energy. According to Noether's theorem, every continuous symmetry of a physical system corresponds to a conserved quantity. The invariance of a system under time translations leads to the conservation of energy, indicating that if the laws of physics do not change over time, the total energy of the system remains constant.

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