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A particle in 1-D moves under the influence of a potential of V(x) a x4, where a is a real constant. For large the quantized energy En depends on as:
  • a)
     
    E∝n4/3
  • b)
    E∝n3/4
  • c)
    E∝n2/3
  • d)
    E∝n3/2
Correct answer is option 'A'. Can you explain this answer?
Most Upvoted Answer
A particle in 1-D moves under the influence of a potential of V(x) a x...
The quantized energy levels for a particle in a 1-dimensional potential can be found by solving the time-independent Schrödinger equation:

[-(h_bar^2/2m) * d^2/dx^2 + V(x)] ψ(x) = E ψ(x)

Given that the potential is V(x) = a x^4, we can substitute this into the Schrödinger equation:

[-(h_bar^2/2m) * d^2/dx^2 + a x^4] ψ(x) = E ψ(x)

To simplify the equation, we can make a change of variables by defining y = x^2. This allows us to rewrite the equation as:

[-(h_bar^2/2m) * (1/4) d^2/dy^2 + a y^2] ψ(y) = E ψ(y)

Now, let's solve this equation. The general solution for ψ(y) can be written as:

ψ(y) = C e^(-α y^2) y^β

where α and β are constants to be determined, and C is a normalization constant.

Plugging this solution into the Schrödinger equation, we get:

[-(h_bar^2/2m) * (1/4) (2β(2β - 1) y^(2β - 2) - 4α y^2) + a y^2] C e^(-α y^2) y^β = E C e^(-α y^2) y^β

Simplifying, we find:

[-(h_bar^2/2m) * β(2β - 1) + a] y^(2β) e^(-α y^2) = E y^(2β) e^(-α y^2)

Since y = x^2, this equation can be rewritten as:

[-(h_bar^2/2m) * β(2β - 1) + a] x^(4β) e^(-α x^2) = E x^(4β) e^(-α x^2)

Dividing both sides by x^(4β) e^(-α x^2), we get:

[-(h_bar^2/2m) * β(2β - 1) + a] = E

This equation determines the quantized energy levels E in terms of the constant a and the parameter β. The value of β can be determined by considering the boundary conditions of the system. Without further information about the system, it is not possible to determine the precise dependence of E on a.
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Community Answer
A particle in 1-D moves under the influence of a potential of V(x) a x...
Concept:
According to WKB approximation:
We have to use the relation that:

where, β12=π/4, for V (x) to be finite a boundary and β12=0 , for V(x) to be infinite at the boundary.
Explanation:
We have a particle in 1-D that moves under the influence of a potential of V(x) a x4.
We use the above formula with β12= π/4 as the potential is finite at the turning points, and we get:

The potential is symmetric hence,
where is some constant
Taking the substitutionwe get:

Now pulling out all the E terms, out and doing the integration we get:
This constant carries a constant after doing the integration.
Now solving it a bit we get:
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A particle in 1-D moves under the influence of a potential of V(x) a x4, where a is a real constant. For largenthe quantized energy Endepends onnas:a)E∝n4/3b)E∝n3/4c)E∝n2/3d)E∝n3/2Correct answer is option 'A'. Can you explain this answer?
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