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)=–mo²x² (where m is the electron mass, ø is a constant angular frequency). In this case, the Schrödinger equation takes the following form, ħ? d°w (x) ¸ 1 -moxy (x)= Ey (x). 2m dx? 2 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, mox? y,(x)= exp| 2h 2mox? v.(x)=| mox -1 exp| 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 @.
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)=–mo²x² (where m is the electron mass, ø is a constant angular frequency). In this case, the Schrödinger equation takes the following form, ħ? d°w (x) ¸ 1 -moxy (x)= Ey (x). 2m dx? 2 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, mox? y,(x)= exp| 2h 2mox? v.(x)=| mox -1 exp| 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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![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)=–mo²x² (where m is the electron mass, ø is a constant angular frequency). In this
case, the Schrödinger equation takes the following form,
ħ? d°w (x) ¸ 1
-moxy (x)= Ey (x).
2m dx?
2
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,
mox?
y,(x)= exp|
2h
2mox?
v.(x)=|
mox
-1 exp|
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%2F2c73beca-60c5-4fd8-bb91-a7d23ee83c12%2F6c05ac71-eb80-4024-8b3e-f20a4595cf64%2Fa9s2f4.png&w=3840&q=75)
Transcribed Image Text: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)=–mo²x² (where m is the electron mass, ø is a constant angular frequency). In this
case, the Schrödinger equation takes the following form,
ħ? d°w (x) ¸ 1
-moxy (x)= Ey (x).
2m dx?
2
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,
mox?
y,(x)= exp|
2h
2mox?
v.(x)=|
mox
-1 exp|
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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