Quantum vs. Classical Mechanic graphing

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SUMMARY

The discussion centers on the relationship between Classical Mechanics and Quantum Mechanics, specifically regarding the potential energy functions used in both frameworks. It establishes that the potential in the Schrödinger's equation is identical to that in classical mechanics, such as V(x)=1/2 k x^2, highlighting that while the equations and interpretations differ, the underlying potential remains consistent. The conversation emphasizes that this consistency does not extend to the behavior of particles in quantum mechanics, where wave functions and charge densities introduce complexities absent in classical mechanics.

PREREQUISITES
  • Understanding of Classical Mechanics principles, particularly potential energy functions.
  • Familiarity with Quantum Mechanics concepts, including the Schrödinger equation.
  • Knowledge of wave functions and their role in Quantum Mechanics.
  • Basic grasp of Quantum Field Theory (QFT) and its implications.
NEXT STEPS
  • Study the implications of the Schrödinger equation in Quantum Mechanics.
  • Explore the differences between classical and quantum potential energy functions.
  • Investigate the role of wave functions in determining charge density in Quantum Mechanics.
  • Learn about Quantum Field Theory and its departure from classical concepts.
USEFUL FOR

Students and professionals in physics, particularly those studying or working in theoretical physics, quantum mechanics, or classical mechanics, will benefit from this discussion.

terp.asessed
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Hey, I am curious if there's a correspondence between Classical and Quantum Mechanics graphs in terms of Potential (or kinetic) Energy as a function of x, aside from equations?
 
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In classical mechanics, particles cause potentials and particles are also affected by potentials. So there some kind of a consistency between them because a particle which is affected by another particle's potential field, can itself have a similar potential field. There are only some cases where you can have potentials which aren't related to some kind of a usual particles configuration, like a uniform electric field which can be caused only by charges at infinity.
But in QM, things are different. The potential used in the Schrödinger's equation is the same as the potential used in classical mechanics and so there is no difference in that sense. But if you want to know the electric potential field of an electron, then things get different. You should use the modulus squared of the electrons' wave function(times -e) as the charge density and find the electric potential but that depends on the wave function's form and so things are very different from classical mechanics here.So different that there can be no comparison in the way you want! Also the consistency I mentioned in the case of classical mechanics isn't present here and I think that's one important reason that pushed physicists for formulating Quantum theories for fields.
In QFT things are even more different!
 
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Thanks for the info! Btw, if you don't mind, could you pls expand on:

Shyan said:
The potential used in the Schrödinger's equation is the same as the potential used in classical mechanics and so there is no difference in that sense.

I thought that it only applied in the case where energy level (n) in the QM is very large to the point the wave behaves more like Classical than Quantum Mechanics?
 
I think its better to explain in using an example. Consider a particle in the potential V(x)=\frac{1}{2} k x^2. As you can see, there is nothing here that tells us we want to do it classically or quantum mechanically. That's exactly what I mean. The procedures, equations, interpretations and solutions are different, but the potential is the same!
You use V(x)=\frac{1}{2} k x^2 for solving the classical problem and when you want to solve the quantum mechanical problem, you use the same thing and you do nothing to make it quantum mechanical!
 
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Ok, thanks!
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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