Questions on WKB approximation

In summary, the WKB (Wentzel-Kramers-Brillouin) approximation is a mathematical method used in quantum mechanics to approximate the solutions to the Schrödinger equation for problems involving rapidly varying potentials. It is important because it allows for approximate solutions to complex systems that cannot be solved exactly. The approximation involves making an educated guess for the wave function based on the potential, and it is only valid for systems with rapidly varying potentials. It is not always accurate, but becomes more accurate for higher energy states and slower varying potentials. However, it does not take into account quantum tunneling effects.
  • #1
jasum
10
0
The description in P.252in liboff's quantum mechanics,

I cannot not figure out the continuity and continue in first order derivative of the wave function
[tex]
\varphi_I = \frac{1}{\sqrt{\kappa}} \exp {(\int_{x_1}^{x} \kappa dx)}
[/tex]

in (7.184)
[tex]
\varphi_{\amalg} = \frac{2}{\sqrt{k}} \exp {(\int_{x_1}^{x} k dx + \pi/4)}
[/tex]

and (7.185)

The potenial is
[tex]
V(x) = E - F_1 (x-x_1)
[/tex]

F1 is a constant
where the boundary is in x1
Thank you!
 
Last edited:
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  • #2


Thank you for your question regarding the continuity and first order derivative of the wave function in P.252 of Liboff's Quantum Mechanics.

Firstly, it is important to understand that the wave function, denoted by the symbol ψ, describes the behavior of a quantum system. In quantum mechanics, the wave function is a complex-valued function that contains all the information about the system, including its position, momentum, and energy. The continuity and first order derivative of the wave function are crucial in understanding the behavior of the system and how it evolves over time.

In equation (7.184), the wave function ψ_I is given as a function of the spatial variable x, with a constant κ in the denominator. This form of the wave function is known as the "incident wave" and describes the behavior of a wave approaching a potential barrier. The term in the exponential, ∫x1x κ dx, represents the phase of the wave and is related to the momentum of the particle. The continuity of this wave function at x=x1 ensures that the wave is continuous as it approaches the potential barrier.

In equation (7.185), the wave function ψ_∏ is given as a function of the spatial variable x, with a constant k in the denominator. This form of the wave function is known as the "transmitted wave" and describes the behavior of a wave that has passed through a potential barrier. The term in the exponential, ∫x1x k dx + ∏/4, represents the phase of the wave and is related to the momentum of the particle. The continuity of this wave function at x=x1 ensures that the wave is continuous as it passes through the potential barrier.

The potential V(x) = E - F_1 (x-x_1) in both equations represents the energy of the particle, with E being the total energy and F_1 being a constant. The boundary at x=x1 in both equations indicates that the potential barrier starts at this point.

In summary, the continuity and first order derivative of the wave function are essential in understanding the behavior of a quantum system, particularly when it interacts with a potential barrier. I hope this helps clarify your understanding. Please let me know if you have any further questions.


 

1. What is the WKB approximation?

The WKB (Wentzel-Kramers-Brillouin) approximation is a mathematical method used in quantum mechanics to approximate the solutions to the Schrödinger equation, which describes the behavior of quantum particles. It is particularly useful for problems involving rapidly varying potentials.

2. Why is the WKB approximation important?

The WKB approximation allows us to find approximate solutions to the Schrödinger equation for complex systems that cannot be solved exactly. It is also used in many areas of physics, including quantum mechanics, optics, and solid-state physics.

3. How does the WKB approximation work?

The WKB approximation involves making an ansatz (educated guess) for the wave function based on the properties of the potential. This ansatz is then substituted into the Schrödinger equation, leading to a differential equation that can be solved using standard techniques. The resulting wave function is an approximation to the exact solution.

4. What are the limitations of the WKB approximation?

The WKB approximation is only valid for systems with rapidly varying potentials. It also assumes that the wave function is slowly varying, which may not be true for some systems. Additionally, it does not take into account quantum tunneling effects.

5. How accurate is the WKB approximation?

The accuracy of the WKB approximation depends on the specific problem and how well the ansatz matches the true wave function. In general, it becomes more accurate for higher energy states and for potentials that vary more slowly. However, it is always an approximation and may not provide an exact solution.

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