Particle Momentum and Position Calculation in Heisenberg Picture

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In summary, the conversation discusses the Heisenberg picture and its application to calculating the momentum of a particle moving under a potential. It mentions the use of the differential equation \frac{dx}{dt}=p/m and the calculation of the expression x(t+\epsilon)-x(t)=p\epsilon/m. The conversation also clarifies that operators and eigenvalues should not be mixed as they are completely different concepts.
  • #1
eljose
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Let,s suppose we have a particle moving under a potential V:
By Heisenberg picture we know that:

[tex]\frac{dx}{dt}=p/m [/tex]

so if we knew x(t) and x(t+h) we could calculate the expresion:

[tex]x(t+\epsilon)-x(t)=p\epsilon/m [/tex]

so knowing x(t) and x(t+e) we could calculate the momentum of the particle:
 
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  • #2
eljose said:
Let,s suppose we have a particle moving under a potential V:
By Heisenberg picture we know that:

[tex]\frac{dx}{dt}=p/m [/tex]

so if we knew x(t) and x(t+h) we could calculate the expresion:

[tex]x(t+\epsilon)-x(t)=p\epsilon/m [/tex]

so knowing x(t) and x(t+e) we could calculate the momentum of the particle:

Please do not mix the differential equation between operators and eigenvalues. They are completely different.


Seratend.
 
  • #3


p=m(x(t+\epsilon)-x(t))/\epsilon

This calculation in the Heisenberg picture allows us to determine the momentum of a particle without directly measuring it. By knowing the position of the particle at two different times, we can calculate the change in position over a small time interval and use it to determine the momentum. This is an important concept in quantum mechanics, as it shows that the position and momentum of a particle cannot be known simultaneously with absolute certainty. The Heisenberg uncertainty principle states that the more precisely we know the position of a particle, the less precisely we can know its momentum, and vice versa. Therefore, the Heisenberg picture provides a way to calculate these quantities without violating this fundamental principle. This is crucial in understanding the behavior of particles at the atomic and subatomic level, where the laws of classical mechanics do not apply.
 

FAQ: Particle Momentum and Position Calculation in Heisenberg Picture

What is the Heisenberg picture in quantum mechanics?

The Heisenberg picture is a mathematical framework used in quantum mechanics to describe the evolution of a quantum system over time. In this picture, the operators that represent physical observables, such as position and momentum, are time-independent, while the state of the system changes with time.

How is particle momentum calculated in the Heisenberg picture?

In the Heisenberg picture, particle momentum is calculated using the Heisenberg equation of motion. This equation describes how the operator representing momentum changes with time, and it is derived from the Schrödinger equation.

What is the uncertainty principle in the Heisenberg picture?

The uncertainty principle in the Heisenberg picture states that the more precisely the position of a particle is known, the less precisely its momentum can be known, and vice versa. This is a fundamental principle in quantum mechanics and is a consequence of the non-commutativity of position and momentum operators.

How does the Heisenberg picture handle the calculation of particle position?

In the Heisenberg picture, the operator representing particle position remains time-independent, while the state of the system changes with time. The position of a particle can be calculated by measuring the corresponding operator on the state of the system at a specific time.

What are the advantages of using the Heisenberg picture in particle momentum and position calculations?

The Heisenberg picture is useful because it allows for the description of the dynamics of a quantum system in a time-independent manner. This makes it easier to analyze and solve problems involving time evolution. Additionally, the Heisenberg picture provides a more intuitive understanding of the uncertainty principle and the relationship between particle momentum and position.

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