A neutron of mass m of energy E < + Vo is in the internucleon potential which can be modeled as shown below: V(x)=∞ E • m x= 0 x= a -Vo I. Write down the Schrödinger equation for: region I (0sxsa, V(x) = -V, ), and region II (x >a ,V(x) = +V, ) II. Estimate the kinetic energy of the nucleons when they reach region II.
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- Consider a particle of mass m moving in one dimension with wavefunction $(x) 2 2πα sin for VI and zero otherwise. Is the wave function an eigenfunction of p? If so, what is the eigenvalue?Problem 1: (a) A non-relativistic, free particle of mass m is bouncing back and forth between two perfectly reflecting walls separated by a distance L. Imagine that the two oppositely directed matter waves associated with this particle interfere to create a standing wave with a node at each of the walls. Find the kinetic energies of the ground state (first harmonic, n = 1) and first excited state (second harmonic, n = 2). Find the formula for the kinetic energy of the n-th harmonic. (b) If an electron and a proton have the same non-relativistic kinetic energy, which particle has the larger de Broglie wavelength? (c) Find the de Broglie wavelength of an electron that is accelerated from rest through a small potential difference V. (d) If a free electron has a de Broglie wavelength equal to the diameter of Bohr's model of the hydrogen atom (twice the Bohr radius), how does its kinetic energy compare to the ground-state energy of an electron bound to a Bohr model hydrogen atom?Subject: Physics - Jr/Senior level Quantum Mechanics - If two wave functions ψ1 (x,t), ψ2 (x,t) are solutions to the (one dimensional) time dependent Schroedinger eqn. show that ψ = Aψ1 + Bψ2 is also a solution, A and B are complex constants. I started by plugging Aψ1 + Bψ2 into the time dependent Schroedinger equation but not sure where to go from there. Thank you!
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- Determine the normalization constant for the following wavefunction. Write an expression for the normalized wavefunction. (8) y=(r/ao)et/2a,No Spacing Heading 1 Normal Aa v A A 困、 Paragraph Styles The action along a path is defined to be: S = [(K.E.-P. E.) dt Determine the physical units of action. Detail Feynman's approach to calculating the probability amplitude for an electron to go from one event A to another B using the "sum over all paths". A'Focus 12 1> 12A neutron of mass m of energy E a,V(x) = Vo ) II. Estimate the kinetic energy of the neutron when they reach region III.