Properties of Wave Functions and their Derivatives

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SUMMARY

The discussion centers on the properties of wave functions and their derivatives, specifically the relationship between the derivatives of a wave function, ψ, and its complex conjugate, ψ*. The first statement regarding the equality of the derivatives, \frac{\partial \psi^*}{\partial x} \frac{\partial^2 \psi}{\partial x^2} = \frac{\partial \psi}{\partial x} \frac{\partial^2 \psi^*}{\partial x^2}, is confirmed to be true. The integration by parts technique is employed to demonstrate that \int \frac{\partial^2 \psi}{\partial x^2} \frac{\partial \psi^*}{\partial x}dx = -\int \frac{\partial \psi}{\partial x} \frac{\partial^2 \psi^*}{\partial x^2}dx, reinforcing the validity of the initial statement.

PREREQUISITES
  • Understanding of wave functions in quantum mechanics
  • Familiarity with complex conjugates and their properties
  • Knowledge of calculus, specifically integration by parts
  • Proficiency in partial derivatives
NEXT STEPS
  • Study the application of the product rule in calculus
  • Explore the implications of complex wave functions in quantum mechanics
  • Learn more about integration techniques in advanced calculus
  • Investigate the role of boundary conditions in wave function behavior
USEFUL FOR

Students and researchers in quantum mechanics, physicists analyzing wave functions, and mathematicians focusing on calculus and differential equations will benefit from this discussion.

Kyle.Nemeth
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Homework Statement


I am unsure if the first statement below is true.

Homework Equations


\frac{\partial \psi^*}{\partial x} \frac{\partial^2 \psi}{\partial x^2}=\frac{\partial^2 \psi}{\partial x^2}\frac{\partial \psi^*}{\partial x} Assuming this was true, I showed that \int \frac{\partial \psi^*}{\partial x} \frac{\partial^2 \psi}{\partial x^2}dx=\int \frac{\partial \psi}{\partial x} \frac{\partial^2 \psi^*}{\partial x^2}dx

The Attempt at a Solution


I am unsure whether it is true due to the fact that \psi and \psi^* may be complex.
 
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The first statement is true. Is your question not
$$\frac{\partial\psi^*}{\partial x}\frac{\partial^2\psi}{\partial x^2} = \frac{\partial\psi}{\partial x}\frac{\partial^2\psi^*}{\partial x^2}?$$
 
That might be my question (although I didn't realize it). Here is what I did,

\int \psi^* \frac{\partial^3 \psi}{\partial x^3}dx=-\int \frac{\partial^2 \psi}{\partial x^2} \frac{\partial \psi^*}{\partial x}dx I used the product rule for the integrand on the left hand side of the equation to show this statement. From here (using the assumption I originally asked about in the OP), I claimed that -\int \frac{\partial^2 \psi}{\partial x^2} \frac{\partial \psi^*}{\partial x}dx=-\int \frac{\partial \psi^*}{\partial x} \frac{\partial^2 \psi}{\partial x^2}dx From here, I used integration by parts by letting u=\frac{\partial \psi^*}{\partial x} and dv=\frac{\partial^2 \psi}{\partial x^2}dx to arrive at the second statement I made in the OP (In the relevant equations section).
 
You could also perform this step immediately by $$
\int \frac{\partial}{\partial x}(\frac{\partial \psi}{\partial x}\frac{\partial \psi^*}{\partial x})dx= \int \frac{\partial^2 \psi}{\partial x^2}\frac{\partial \psi^*}{\partial x}dx+\int \frac{\partial \psi}{\partial x}\frac{\partial^2 \psi^*}{\partial x^2}dx$$
Because the L.H.S. is equal to zero at the infinities, we obtain $$
\int \frac{\partial^2 \psi}{\partial x^2}\frac{\partial \psi^*}{\partial x}dx=-\int \frac{\partial \psi}{\partial x}\frac{\partial^2 \psi^*}{\partial x^2}dx$$
 
I apologize for not replying to this post. Thanks IanBerkman, you've been very helpful.
 

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