Multi-Electron Atoms Flashcards

1
Q

What is the problem with multi-electron atoms?

A

We cannot solve the TISE analytically for many electrons - we need approximations.

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2
Q

What is the ludicrously independent electron approximation?

A

Each electron in a multi-electron atom has a hydrogen-like wave function independent of all the others.

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3
Q

What is the equation for the energy in the ludicrously independent electron approximation?

A

En = -Z^2/n^2 *E(Ry)

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4
Q

What is meant by ionisation energy?

A

Energy needed to remove most weakly bound electron from an atom.

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5
Q

What happens to the electrons in the ludicrously independent electron approximation?

A

All electrons would occupy lowest n=1 state: 1s.

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6
Q

What do we need to correct in the ludicrously independent electron approximation?

A

More than 1 electron cannot occupy the same quantum state (n, l, j, m(j)) in an atom.

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7
Q

Which order do we fill up the available quantum states?

A

From high binding energy to low.

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8
Q

How does the spin fill up when increasing electron number?

A

Fills up with up spin then fills with down spin (so if has 3 parts, will fill up with 3 ups then 3 downs).

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9
Q

Where do the groups appear on the periodic table?

A

Right hand side.

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10
Q

Where do the transition elements appear on the periodic table?

A

Middle.

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11
Q

Describe inert gases.

A

Filled shell - stable and unreactive.

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12
Q

Describe alkali metals.

A

Filled shells + 1 electron. Easy to ionise by losing outer electron.

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13
Q

Describe the halogens.

A

1 electron short of a filled shell -> they like to acquire an electron e.g Cl + e(+) -> Cl(-)

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14
Q

What is the central field approximation?

A

Electrons move in a potential due to the nucleus screened by all electrons in more inner shells.

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15
Q

At different distance r outside an electron with 3 protons and 2 electrons orbiting, what does an electron see?

A

A large enough r, electrons sees 1+ only (3+ + 2-). At low r an electron sees 3+

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16
Q

What is the screened potential?

A

No longer 1/r -> need to tweak R(r).

17
Q

What is Hund’s first rule?

A

Spins prefer to be aligned rather than anti-aligned or paired.

18
Q

Why is Hund’s rule a thing?

A

Total Ψ has to be antisymmetric: Ψ = Ψ(spin)*Ψ(space) -> symmetric Ψ(spin) must go with antisymmetric Ψ(space) and vice versa.

19
Q

What is the Pauli Exclusion Principle?

A

No two electrons in an atom can have the same set of quantum numbers.

20
Q

What is meant by exchange symmetry?

A

When |Ψ(r1,r2)|^2 = |Ψ(r2, r1)|^2 -> because electrons are indistinguishable.

21
Q

How can we use exchange symmetry to determine whether a particle is a boson or a fermion?

A

If exchange symmetry is even then they’re bosons, if odd then fermions (odd if Ψ(r1,r2) = -Ψ(r2,r1)