Ignoring the fine structure splitting, hyperfine structure splitting, etc., such that energy levels depend only on the principal quantum number n, how many distinct states of singly-ionized helium (Z = 2) have energy E= -13.6 eV? Write out all the quantum numbers (n, l, m, m,) describing each distinct state. (Recall that the ground state energy of hydrogen is E₁ = -13.6 eV, and singly-ionized helium may be treated as a hydrogen-like atom.)
Ignoring the fine structure splitting, hyperfine structure splitting, etc., such that energy levels depend only on the principal quantum number n, how many distinct states of singly-ionized helium (Z = 2) have energy E= -13.6 eV? Write out all the quantum numbers (n, l, m, m,) describing each distinct state. (Recall that the ground state energy of hydrogen is E₁ = -13.6 eV, and singly-ionized helium may be treated as a hydrogen-like atom.)
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![**Problem 7: Quantum States of Singly-Ionized Helium**
*Ignoring the fine structure splitting, hyperfine structure splitting, etc., such that energy levels depend only on the principal quantum number \( n \), how many distinct states of singly-ionized helium (\( Z = 2 \)) have energy \( E = -13.6 \, \text{eV} \)? Write out all the quantum numbers \( (n, \ell, m_\ell, m_s) \) describing each distinct state. (Recall that the ground state energy of hydrogen is \( E_1 = -13.6 \, \text{eV} \), and singly-ionized helium may be treated as a hydrogen-like atom.)*
**Explanation:**
This problem involves finding the distinct quantum states for singly-ionized helium where the energy level is described only by the principal quantum number \( n \). It assumes a simplified model of atom where other effects such as fine structure are ignored.
1. **Quantum Numbers**:
- \( n \): Principal quantum number.
- \( \ell \): Orbital angular momentum quantum number, which can take values from \( 0 \) to \( n-1 \).
- \( m_\ell \): Magnetic quantum number, with values from \( -\ell \) to \( \ell \).
- \( m_s \): Spin quantum number, which can be \( +\frac{1}{2} \) or \( -\frac{1}{2} \).
2. **Energy Level Consideration**:
- Since \( Z = 2 \) for helium, and the problem mentions \( E = -13.6 \, \text{eV} \), this corresponds to the \( n=2 \) energy level, because for hydrogen-like atoms, \( E_n = -13.6 \, \text{eV} \times \frac{Z^2}{n^2} \).
- For \( Z = 2 \), \( E_1 = -54.4 \, \text{eV} \). For \( n=2 \), \( E_2 = -13.6 \, \text{eV} \).
3. **Quantum States Enumeration**:
- For \( n=2 \): \( \ell \) can be \( 0 \) or \( 1 \).
- If](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F62a79166-ba2c-43d7-9fa1-94c5c5be2063%2F28f10c04-b6d8-4749-8f12-35be46f0b9e9%2Fe8tadsk_processed.png&w=3840&q=75)
Transcribed Image Text:**Problem 7: Quantum States of Singly-Ionized Helium**
*Ignoring the fine structure splitting, hyperfine structure splitting, etc., such that energy levels depend only on the principal quantum number \( n \), how many distinct states of singly-ionized helium (\( Z = 2 \)) have energy \( E = -13.6 \, \text{eV} \)? Write out all the quantum numbers \( (n, \ell, m_\ell, m_s) \) describing each distinct state. (Recall that the ground state energy of hydrogen is \( E_1 = -13.6 \, \text{eV} \), and singly-ionized helium may be treated as a hydrogen-like atom.)*
**Explanation:**
This problem involves finding the distinct quantum states for singly-ionized helium where the energy level is described only by the principal quantum number \( n \). It assumes a simplified model of atom where other effects such as fine structure are ignored.
1. **Quantum Numbers**:
- \( n \): Principal quantum number.
- \( \ell \): Orbital angular momentum quantum number, which can take values from \( 0 \) to \( n-1 \).
- \( m_\ell \): Magnetic quantum number, with values from \( -\ell \) to \( \ell \).
- \( m_s \): Spin quantum number, which can be \( +\frac{1}{2} \) or \( -\frac{1}{2} \).
2. **Energy Level Consideration**:
- Since \( Z = 2 \) for helium, and the problem mentions \( E = -13.6 \, \text{eV} \), this corresponds to the \( n=2 \) energy level, because for hydrogen-like atoms, \( E_n = -13.6 \, \text{eV} \times \frac{Z^2}{n^2} \).
- For \( Z = 2 \), \( E_1 = -54.4 \, \text{eV} \). For \( n=2 \), \( E_2 = -13.6 \, \text{eV} \).
3. **Quantum States Enumeration**:
- For \( n=2 \): \( \ell \) can be \( 0 \) or \( 1 \).
- If
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