Lectures 1&2 (Basics, FM & Bohr-van Leeuwen) Flashcards

1
Q

What is magnetisation?

A

Response of a material due to an applied magnetic field

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2
Q

Flux density inside solenoid?

A

B = µ0 IN/L

(so H = IN/L)

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3
Q

Magnetic moment equation?

A

µ = MV

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4
Q

µ units?

A

Am^2

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5
Q

Angular momentum equation for an electron?

A

l = m_e * r x v

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6
Q

How is M defined?

A

Magnetic moment per unit volume

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7
Q

Show that magnetic moment µ can be given in terms of the angular momentum l of the electron

A

l = m_e * r x v

and µ = -e/2 * r x v

µ = - e/2m * l

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8
Q

Equation for µ in terms of orbital angular momentum?

A

µ = γl

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9
Q

γ value?

A

γ = -e/2m or -ge/2m for > 1 electron

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10
Q

Show that Bohr magneton comes from magnetic moment and orbital angular momentum

A

µ = -e/2m * l

µ_z = -e/2m * m_l * ℏ

µ_B = eℏ/2m

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11
Q

Show that µ = µ0(1+X)

A

B = µ0(H+M) = µ0(H+XH) = µ0H(1+X) = µH

where µ = µ0(1+X)

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12
Q

Which materials experience diamagnetism?

A

All

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13
Q

Susceptibility of a diamagnet?

A

X < 0

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14
Q

How do diamagnets react to magnetic fields?

A

Weakly repelled

(A small opposite moment is induced due to Lenz’s law)

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15
Q

What gradient does a diamagnet have on the M vs H graph?

A

-ve

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16
Q

Susceptibility of a paramagnet?

A

X > 0

17
Q

How do paramagnets react to magnetic fields?

A

Weakly attracted

Moments not aligned in absence of H_ext

18
Q

Which materials experience paramagnetism?

A

Those with net angular momentum on each atom

19
Q

Why does a FM remain magnetised at H=0?

A

Exchange interaction and anisotropy

20
Q

X of FM?

A

X_eff = ∂M/∂H

21
Q

What is Ms?

A

Magnetisation of the sample when all domains are aligned and characteristic of the material

22
Q

What is Mr?

A

Remanent magnetisation is that at zero field, and can depend on the sample

23
Q

What is Hc?

A

The coercive field (coercivity) is the reverse field that needs to be applied to zero magnetisation

24
Q

What is Mr/Ms?

A

Remanent fraction / loop squareness

25
Q

What is work density in a hysteresis loop?

A

µ0 ∫M.dH

= energy lost in the material by going around the loop

26
Q

Spin and orbital magnetic moment equations?

A

µ_z,l = -e/2m * m_l * ℏ

µ_z,s = -e/m * m_s * ℏ

27
Q

What does a skinny hysteresis loop mean?

A

Less energy lost

28
Q

Why is Permalloy good for magnetic recording?

A

Easily magnetisable (soft)

29
Q

What properties are good for permanent magnets?

A

High Ms and large Hc

30
Q

Are Ms, Hc and Mr sample independent?

A

Only Ms

31
Q

Does Ms depend on T?

A

Yes

32
Q

When does Ms vanish?

A

At Tc - above which material becomes paramagnetic

33
Q

What does the Bohr-van Leeuwen theorem show?

A

According to classical physics, there is no interaction between an applied field and the electrons in a material

34
Q

Brief steps to show the BvL theorem?

A

(Model material as system of charges. Check affect of H as to whether M induced)

Electron energy: E = -µ.B = -µ.µ0H = -µBcosø

But m. field means Lorentz force F = q(E + vxB) - so the B always produces forces perp. to the velocity

No work is done by the magnetic field, so there is no change in energy

So µ ~ E/B doesn’t depend on m. field

35
Q

How can exchange energy be estimated?

A

kTc

36
Q

Why is there a discrepancy form g=2?

A

Because interactions are due to virtual photons. Electrons emit and reabsorb virtual photons if µ is measured during the lifetime of a virtual photon there is an extra orbital component