Lectures 3&4 (Exchange & Heisenberg Hamiltonian) Flashcards

1
Q

How did Weiss attempt to explain FM?

A

1) Molecular / exchange field that aligns all m. moments (explains M(T))

2) Magnetic moments where M direction varies from one domain to the next (explains hysteresis loops)

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2
Q

What energy is from magnetic dipole interaction?

A

Magnetostatic

(energy between 2 magnetic moments)

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3
Q

What energy is from Coulomb interaction?

A

Electrostatic

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4
Q

Difference of r between parallel and antiparallel spins?

A

AP can occupy same orbital - r lower - higher energy (Coulomb)

P can’t occupy same orbital - r lower

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5
Q

Do P or AP spins have higher energy, following from Coulomb?

A

P lower energy than AP

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6
Q

In terms of spin, what do we want for FM?

A

Neighbouring spins ||

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7
Q

Hund’s first rule?

A

Maximise spin to obtain lowest energy

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8
Q

Will the overall 2-fermion wavefunction be symmetric?

A

No, antisymmetric

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9
Q

Which direction are spins in a symmetric spin wavefunction?

A

Symmetric

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10
Q

How does particle exchange manifest in the determinant?

A

Switching 2 columns (i.e. switching the positions of the 2 electrons)

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11
Q

In exchange, when will the wavefunction =0?

A

When any 2 rows/columns are equal

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12
Q

What is the symmetry of the overall wavefunction?

A

Antisymmetric

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13
Q

What does it mean physically, that a wavefunction is antisymmetric?

A

Is it not the same after exchange

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14
Q

What is the symmetric version of ø, before and after exchange?

A

Before:
ø = 1/√2 [ø_α(1)ø_β(2) + ø_α(2)ø_β(1)]

After:
ø = 1/√2 [ø_α(2)ø_β(1) + ø_α(1)ø_β(2)]

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15
Q

What is the antisymmetric version of ø, before and after exchange?

A

Before:
ø = 1/√2 [ø_α(1)ø_β(2) - ø_α(2)ø_β(1)]

After:
ø = 1/√2 [ø_α(2)ø_β(1) - ø_α(1)ø_β(2)]

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16
Q

What is the ø wavefunction?

A

Represent atomic orbitals i.e., positions of the electrons in space

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17
Q

Is the ø wavefunction discrete or continuous?

A

Continuous

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18
Q

Is the X wavefunction discrete or continuous?

A

Discrete

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19
Q

Why do we make spin point either up or down?

A

Can point anywhere - but we define a quantization axis (z-axis)

Measure projection of angle along z i.e., above horizontal = spin up

20
Q

What is the singlet state?

A

Antisymmetric spin eigenstate

21
Q

What spins does the antisymmetric spin eigenstate correspond to?

A

Antiparallel spins

22
Q

When is the antisymmetric singlet state permitted?

A

When 2 electrons are in the same spatial state (same orbital)

23
Q

How many electrons would doublets need?

A

3 electrons (for spin +/- 1/2)

24
Q

What is the overall wavefunction for the singlet state?

A

1/√2 [ø_α(1)ø_β(2) + ø_α(2)ø_β(1)] * X_S

25
Q

What is the overall wavefunction for the triplet state?

A

1/√2 [ø_α(1)ø_β(2) - ø_α(2)ø_β(1)] * X_T

26
Q

What question do we ask to define the exchange integral?

A

How much energy do we save when doing from antiparallel to parallel spins?

27
Q

How much energy do we save going from AP to P spins?

A

E_S - E_T / 2 = exchange integral

28
Q

How can the exchange integral be defined?

A

E_S - E_T / 2

29
Q

How is the energy from AP to P states defined (exchange energy)?

A

E = U_elec +/- J

30
Q

For J itself +ve, what do +/- J correspond to?

A

+J = AP (singlet state)

-J = P (triplet state)

31
Q

For J itself -ve, what do +/- J correspond to?

A

+J = P (triplet state)

-J = AP (singlet state)

32
Q

What is the exchange integral J physically?

A

A correction to the classical Coulomb interaction which accounts for the PEP

33
Q

When do spins of the same sign cost and save energy?

A

Cost energy when close, save it when further apart

34
Q

In terms of J, when does AFM occur?

A

When J itself is -ve

35
Q

How do electrons being on the same / neighbouring atoms affect J?

A

Same atom - J usually +ve (FM)

Neighbouring - molecular orbitals instead of atomic. Anti-bonding more energetically costly due to higher curvature so KE. Singlet favoured to J likely -ve

36
Q

What are the types of molecular orbital?

A

Bonding / anti-bonding

37
Q

Why is J likely negative if electrons are in neighbouring atoms?

A

Anti-bonding orbital (P spins) higher energy since spatial wavefunction has higher curvature and KE so singlet state (AP) is favoured

38
Q

When might indirect exchange occur?

A
39
Q

What does it mean, that the 2 electrons in exchange are tunneling?

A

The 2 electrons constantly change places

40
Q

Can electrons in singlet / triplet states occupy the same space?

A

Singlet electrons can, triplet cannot since the wavefunction goes to 0 as r1 -> r2

41
Q

What is the exchange interaction (in terms of swapping spins)?

A

When we swap 2 parallel spins, the sign of ø (and 𝚿) changes and the energy cost of electrostatic repulsion is minimised

42
Q

Types of exchange?

A
  • Intra-atomic - direct (Hund’s rules)
  • Inter-atomic - direct (molecules), indirect (rare earths), superexchange
  • s-d - direct, band mixing
  • Itinerant - direct (Fe, Co, Ni)
43
Q

What is superexchange?

A

Indirect exchange between non-neighbouring magnetic ions mediated by a non-magnetic ion in between

44
Q

Is intra-atomic exchange direct? Is preferred state P or AP?

A

Direct, P

45
Q

Is inter-atomic exchange direct? Is preferred state P or AP?

A

Molecules - direct, AP

Indirect - rare earth, P

Superexchange - indirect, AP

46
Q

Is s-d interaction direct? Is preferred state P or AP?

A

Direct, P

47
Q

Is itinerant exchange direct? Is preferred state P or AP?

A

Direct, P