3. The quantum harmonic oscillator is the quantum-mechanical analog of the classical harmonic oscillator. Because an arbitrary potential can usually be approximated as a harmonic potential at the vicinity of a stable equilibrium point, it is one of the most important model systems in quantum mechanics. Consider an electron trapped by a one-dimensional harmonic potential V (x)=-mox² (where m is the electron mass, o is a constant angular frequency). In this case, the Schrödinger equation takes the following form, h d'y(x)¸ 1mo³x*w (x)= Ew (x). 2m dx? The electron is initially trapped at the ground level. After absorbing a photon, it transits to an excited level. The wave functions of the ground and excited levels take the following forms, respectively, тоx W;(x) = exp| 2h 2mox w.(x) = тох? —1 |еxp 2h Determine the energy of the electron at the ground and excited levels, respectively, and therefore express the wavelength of the incident photon in terms of @.
3. The quantum harmonic oscillator is the quantum-mechanical analog of the classical harmonic oscillator. Because an arbitrary potential can usually be approximated as a harmonic potential at the vicinity of a stable equilibrium point, it is one of the most important model systems in quantum mechanics. Consider an electron trapped by a one-dimensional harmonic potential V (x)=-mox² (where m is the electron mass, o is a constant angular frequency). In this case, the Schrödinger equation takes the following form, h d'y(x)¸ 1mo³x*w (x)= Ew (x). 2m dx? The electron is initially trapped at the ground level. After absorbing a photon, it transits to an excited level. The wave functions of the ground and excited levels take the following forms, respectively, тоx W;(x) = exp| 2h 2mox w.(x) = тох? —1 |еxp 2h Determine the energy of the electron at the ground and excited levels, respectively, and therefore express the wavelength of the incident photon in terms of @.
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![3. The quantum harmonic oscillator is the quantum-mechanical analog of the classical harmonic
oscillator. Because an arbitrary potential can usually be approximated as a harmonic potential
at the vicinity of a stable equilibrium point, it is one of the most important model systems in
quantum mechanics. Consider an electron trapped by a one-dimensional harmonic potential
V (x)=-mox² (where m is the electron mass, o is a constant angular frequency). In this
case, the Schrödinger equation takes the following form,
h d'y(x)¸ 1mo³x*w (x)= Ew (x).
2m dx?
The electron is initially trapped at the ground level. After absorbing a photon, it transits to an
excited level. The wave functions of the ground and excited levels take the following forms,
respectively,
тоx
W;(x) = exp|
2h
2mox
w.(x) =
тох?
—1 |еxp
2h
Determine the energy of the electron at the ground and excited levels, respectively, and
therefore
express
the wavelength of the incident photon in terms of @.](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F8c98dcee-ed74-496f-9213-19129a8e97ed%2F1d3f8dca-3f77-41ed-816e-291078912857%2Fm0viqdl.png&w=3840&q=75)
Transcribed Image Text:3. The quantum harmonic oscillator is the quantum-mechanical analog of the classical harmonic
oscillator. Because an arbitrary potential can usually be approximated as a harmonic potential
at the vicinity of a stable equilibrium point, it is one of the most important model systems in
quantum mechanics. Consider an electron trapped by a one-dimensional harmonic potential
V (x)=-mox² (where m is the electron mass, o is a constant angular frequency). In this
case, the Schrödinger equation takes the following form,
h d'y(x)¸ 1mo³x*w (x)= Ew (x).
2m dx?
The electron is initially trapped at the ground level. After absorbing a photon, it transits to an
excited level. The wave functions of the ground and excited levels take the following forms,
respectively,
тоx
W;(x) = exp|
2h
2mox
w.(x) =
тох?
—1 |еxp
2h
Determine the energy of the electron at the ground and excited levels, respectively, and
therefore
express
the wavelength of the incident photon in terms of @.
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