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Many-electron Atoms and Coupling Schemes Questions and Answers

11.

Auger electron emission cannot be obtained from :

Exam Year(s)

MH SET - 2020, SET Exam - 2020,

Answer: D

Auger emission cannot be obtained from hydrogen.

The Auger process needs three electrons: an inner-shell vacancy is created, an electron from a higher level drops into it, and the energy released ejects a third electron (the Auger electron) instead of emerging as an X-ray. An atom must therefore have electrons in at least two shells, at least three in all.

Hydrogen has only one electron (and helium only two), so neither can emit Auger electrons. Carbon, oxygen and nickel have enough electrons; carbon and oxygen Auger lines are in fact standard signals in Auger electron spectroscopy of surfaces.

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12.

\(Eu^{3+}\) ion has outer electronic configuration \(4f^{6}5s^{2}5p^{6}\). Its ground state is characterized by one of the following spectroscopic terms :

Exam Year(s)

MH SET - 2023, SET Exam - 2023,

Answer: A

The ground state of \(Eu^{3+}\) is \({}^{7}F_{0}\).

Apply Hund's rules to the six 4f electrons:

  1. Maximum spin: all six spins parallel in different orbitals, so S = 3 and 2S + 1 = 7.
  2. Maximum L: they occupy \(m_{l}\) = 3, 2, 1, 0, -1, -2, so L = 3, an F term.
  3. The shell is less than half full (six of fourteen), so J = |L - S| = 0.

The term is \({}^{7}F_{0}\). \({}^{8}S_{7/2}\) is the ground state of a half-filled \(4f^{7}\) shell, as in \(Gd^{3+}\) or \(Eu^{2+}\). \({}^{7}F_{6}\) has the J value for a more than half-filled shell, as in \(Tb^{3+}\) (\(4f^{8}\)), and \({}^{6}H_{15/2}\) is the ground state of \(Dy^{3+}\) (\(4f^{9}\)).

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13.

Mn3+ ion has four 3d electrons. The spectroscopic term factor of this ion is :

Exam Year(s)

MH SET - 2024, SET Exam - 2024,

Answer: D

The ground term is \({}^{5}D_{0}\).

Apply Hund's rules to \(3d^{4}\):

  • Maximum S: four parallel spins, \(S = 2\), multiplicity \(2S + 1 = 5\).
  • Maximum L for that S: \(m_{l} = 2, 1, 0, -1\), so \(L = 2\), a D term.
  • The shell is less than half full, so \(J = |L - S| = 0\).

The term is \({}^{5}D_{0}\). \({}^{1}D_{2}\) has the wrong spin, and the terms with half-integer J require an odd number of electrons.

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14.

Assuming that the L-S coupling scheme is valid, the number of permitted transitions from \({}^{2}P_{3/2} \rightarrow {}^{2}S_{1/2}\) due to a weak magnetic field is :

Exam Year(s)

MH SET - 2024, SET Exam - 2024,

Answer: C

There are 6 permitted transitions.

In a weak field, \({}^{2}P_{3/2}\) splits into four levels (\(M_{J} = \pm 3/2, \pm 1/2\), \(g = 4/3\)) and \({}^{2}S_{1/2}\) into two (\(M_{J} = \pm 1/2\), \(g = 2\)). The selection rule \(\Delta M_{J} = 0, \pm 1\) allows:

  • from \(+3/2\): to \(+1/2\) only
  • from \(+1/2\): to \(+1/2\) and \(-1/2\)
  • from \(-1/2\): to \(+1/2\) and \(-1/2\)
  • from \(-3/2\): to \(-1/2\) only

That is 6 transitions, the anomalous Zeeman pattern of the \(D_{2}\) line. 4 is the count for \({}^{2}P_{1/2} \to {}^{2}S_{1/2}\), and 2 or 10 do not fit the selection rule.

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