Magnetics- Ferromagnetism Flashcards

1
Q

How are magnetic moments aligned in ferromagnetic materials?

A

Their neighbouring atoms have aligned magnetic moments even under zero applied magnetic field

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

What gives rise to atomic magnetic moments?

A

Unpaired electrons in the electronic configuration

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

What is Pauli exclusion principle?

A

Interacting electrons must have a different set of quantum numbers.
Alternatively, the overall wave function of a system must be anti-symmetric

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

What are the 4 quantum numbers, n, l, ml, s for electrons?

A

n is principle
l is angular momentum
ml is magnetic
s is spin

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

What is true about spatial symmetry for 2 electrons?

A

If they are spatially symmetric, there is region of constructive interference so spins must be anti-symmetric (opposite).
If they are spatially anti-symmetric, there is region of destructive interference so spins must be symmetric (aligned).

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

Spatially symmetric total spin and spin angular momentum

A

Total spin is S=0
Spin angular momentum ls=2S+1=1
This is singlet state

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

Spatially anti-symmetric total spin and spin angular momentum

A

S=1/2+1/2=1
ls=2S+1=3
This is triplet state

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

Why do symmetric and anti-symmetric configurations have different overall energies?

A

Electrons are electrically charged so have an electrostatic interaction. Different spatial arrangement of electrons mean a difference in electrostatic energy. Therefore the different configurations have different overall energies. This is called the exchange energy.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

What does sign of exchange energy depend on?

A

Meaning whether S=0 or S=1 has a lower energy.
Depends on separation of atoms
Closely spaced atoms have electrons concentrated between them requiring symmetric wave functions and opposite spins so S=0.
Widely spaced atoms have electrons separated from region between them requiring anti-symmetric wavefunctions and aligned spins S=1

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

Bethe-Slater curve

A

Shows dependence of exchange energy with interatomic spacing.
y axis Jex (exchange constant) and x axis interatomic separation.
Line curves up from below x axis to peak above it then curves back down exponentially. Above is ferromagnetic alignment (aligned atomic moments). Below is anti-ferromagnetic alignment (oppositely aligned atomic moments).

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

Formula for exchange energy

A

Eex =-2JexS1•S2
S1 and S2 are spin vectors dot producted together
Jex is positive for ferromagnetic materials

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

What happens if exchange constant Jex is negative?

A

Anti-ferromagnetic: equal opposite adjacent moments mean no net magnetisation at zero field
Ferrimagnetic: unequal opposite adjacent moments mean overall net magnetisation but weaker than ferromagnets.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

What does exchange energy do?

A

It acts to stabilise a particular atomic arrangement of atomic moments

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

Comparing susceptibilities of ferromagnets, ferrimagnets, antiferromagnets, paramagnets and diamagnets on M vs H graph

A

All through origin. Ferromagnet highest gradient as χ»0, then ferrimagnet with lower χ. Then antiferromagnet with χ of 10 to 100. The. Paramagnet with χ>0 still. Then diamagnet with χ<0 and shallowest gradient magnitude.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

Common crystal structures of iron, nickel and cobalt

A

Iron BCC
Nickel FCC
Cobalt HCP

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

What is spin-orbit coupling?

A

Atomic magnetic moments interact with charge of atomic nuclei. Means there are preferred crystallographic orientations for magnetisation. Principle known as magnetocrystalline anisotropy.

17
Q

Easy and hard axes for BCC, FCC, HCP

A

BCC: easy is 100 (along an edge), hard is 111 (through diagonal)
FCC: easy is 111, hard is 100
HCP: easy is 1000 (up through centre), hard is 1010 (from centre of bottom face out equally between 2 atoms on same face)

18
Q

What does easy and hard axis mean?

A

Easy is direction magnetisation prefers. Hard is least preferred as is energetically most costly

19
Q

M vs H graph for easy axis and hard axis

A

Easy rapidly gets to saturation at low applied fields and stays there. Takes hard longer and stronger applied field to get to saturation

20
Q

Formulae for directional cosines of vector M in cubic anisotropy

A

See page 23 lecture 3

21
Q

Formula for magnetocrystalline anisotropy energy density, Ea/V for cubic anisotropy

A

See page 24 lecture 3

22
Q

What magnetocrystalline anisotropy energies are in preferred direction?

A

Low values of energy

23
Q

Formula for magnetocrystalline anisotropy energy density, Ea/V for uniaxial anisotropy

A

See page 26 lecture 3

24
Q

How to find energy to rotate from different crystallographic directions

A

Difference in energy density of one - that of other gives energy density change

25
Q

Hard magnetic materials

A

Ferromagnets for which high magnetic fields needed to change magnetisation because they have strong magnetocrystalline anisotropy (high K numbers in formulae)

26
Q

Soft magnetic materials

A

Ferromagnets for which only weak magnetic fields needed to change magnetisation because they have weak magnetocrystalline anisotropy (low K numbers in formulae)

27
Q

Response of paramagnets to applied magnetic field

A

The magnetic moments gradually rotate into the field direction

28
Q

Response of ferromagnets to applied magnetic field

A

Magnetic domains parallel to field expand and others shrink.

29
Q

Response of anti-ferromagnets to applied magnetic field

A

Magnetic moments gradually rotate into field direction but spring back when the field is removed

30
Q

Response of ferrimagnets to applied magnetic field

A

At low fields: behaves like ferromagnet
High fields: behaves like an anti-ferromagnet with the low moment sub-lattice gradually rotating into the field direction