Lectures 3&4 (Exchange & Heisenberg Hamiltonian) Flashcards

(47 cards)

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
What is the overall wavefunction for the triplet state?
1/√2 [ø_α(1)ø_β(2) - ø_α(2)ø_β(1)] * X_T
26
What question do we ask to define the exchange integral?
How much energy do we save when doing from antiparallel to parallel spins?
27
How much energy do we save going from AP to P spins?
E_S - E_T / 2 = exchange integral
28
How can the exchange integral be defined?
E_S - E_T / 2
29
How is the energy from AP to P states defined (exchange energy)?
E = U_elec +/- J
30
For J itself +ve, what do +/- J correspond to?
+J = AP (singlet state) -J = P (triplet state)
31
For J itself -ve, what do +/- J correspond to?
+J = P (triplet state) -J = AP (singlet state)
32
What is the exchange integral J physically?
A correction to the classical Coulomb interaction which accounts for the PEP
33
When do spins of the same sign cost and save energy?
Cost energy when close, save it when further apart
34
In terms of J, when does AFM occur?
When J itself is -ve
35
How do electrons being on the same / neighbouring atoms affect J?
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
What are the types of molecular orbital?
Bonding / anti-bonding
37
Why is J likely negative if electrons are in neighbouring atoms?
Anti-bonding orbital (P spins) higher energy since spatial wavefunction has higher curvature and KE so singlet state (AP) is favoured
38
When might indirect exchange occur?
39
What does it mean, that the 2 electrons in exchange are tunneling?
The 2 electrons constantly change places
40
Can electrons in singlet / triplet states occupy the same space?
Singlet electrons can, triplet cannot since the wavefunction goes to 0 as r1 -> r2
41
What is the exchange interaction (in terms of swapping spins)?
When we swap 2 parallel spins, the sign of ø (and 𝚿) changes and the energy cost of electrostatic repulsion is minimised
42
Types of exchange?
* 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
What is superexchange?
Indirect exchange between non-neighbouring magnetic ions mediated by a non-magnetic ion in between
44
Is intra-atomic exchange direct? Is preferred state P or AP?
Direct, P
45
Is inter-atomic exchange direct? Is preferred state P or AP?
Molecules - direct, AP Indirect - rare earth, P Superexchange - indirect, AP
46
Is s-d interaction direct? Is preferred state P or AP?
Direct, P
47
Is itinerant exchange direct? Is preferred state P or AP?
Direct, P