Solving Double Square Well Potential - Physical Chemistry Homework

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SUMMARY

The discussion focuses on calculating the time constant τ for an electron in a double square well potential with specific parameters: width L = 2 Bohr, depth V̄ = 4, and separation R = 3, using atomic units. The energy difference ΔE is derived from the quantum states of the electron, calculated using the formula E_n = n²ħ²π² / (2mL²). The final result for τ is τ = h / ΔE, which simplifies to τ = π²ε₀² after substituting the values for ΔE.

PREREQUISITES
  • Understanding of quantum mechanics, specifically quantum states and energy levels.
  • Familiarity with the double square well potential concept.
  • Knowledge of atomic units and their application in physical chemistry.
  • Proficiency in using the formula for energy in a one-dimensional box: E_n = n²ħ²π² / (2mL²).
NEXT STEPS
  • Study the derivation of energy levels in quantum mechanics, focusing on one-dimensional potentials.
  • Learn about the implications of the double square well potential in quantum tunneling.
  • Explore the concept of time constants in quantum systems and their physical significance.
  • Investigate the use of atomic units in various physical chemistry problems.
USEFUL FOR

Students and researchers in physical chemistry, particularly those studying quantum mechanics and potential energy problems, will benefit from this discussion.

ywkim880801
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this is one of my pchem class homework...
and I have no idea how to solve this...

compute [tex]\tau[/tex] for and electron in the double square well potential of width L = 2 Bohr, and depth [tex]\bar{V}[/tex] = 4 and separation R = 3. Use atomic units for your computation...

and in his lecture notes... he gave us (tau) = h/[tex]\DeltaE[/tex] .

he said it's just a simple plug-in problem... but i don't know where that [tex]\DeltaE[/tex]

comes from...

please help me...

pchem sucks...
 
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The energy difference \DeltaE in this problem is the difference between the energies of the two quantum states that are separated by the double square well potential. To calculate this, you can use the equation for the energy of an electron in a one-dimensional box: E_n = n^2 \hbar^2 \pi^2 / (2mL^2)Where n is an integer indicating which quantum state the electron is in. For the lower state, n will be equal to 1, and for the higher state, n will be equal to 2. Thus, the energy difference \DeltaE between these two states is given by: \DeltaE = E_2 - E_1 = \hbar^2 \pi^2 / (2mL^2)Substituting in the given values of L, m, and \hbar, we get:\DeltaE = 4 \pi^2 \hbar^2 / (2 \cdot 2 \cdot (4 \pi \epsilon_0)^2 ) = 4 / (4 \pi \epsilon_0)^2Now that we have \DeltaE, we can plug it into the equation for \tau:\tau = h / \DeltaE = (4 \pi \epsilon_0)^2 / 4 = \pi^2 \epsilon_0^2
 

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