Nuclear Binding and Structure Flashcards

1
Q

What is the binding energy?

A

The energy required to separate nucleons into individual protons and neutrons -> binding energy, E(B)

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2
Q

What is the equation for E(B)?

A

E(B) = (Z(m(p)+m(e)) + Nm(n) - M)*c^2

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3
Q

What is the nuclear force?

A

For binding protons and neutrons despite the electrostatic repulsion of protons - this is the strong interaction.

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4
Q

What are 4 characteristics of the strong interaction?

A
  • Independent of charge
  • Short-ranged ~10^-15 m
  • Nuclear matter nearly const density which suggest that each nucleon interacts with the other nucleons only in its immediate vicinity
  • Nuclear force favours binding of pairs of protons (up and down) or neutrons (up and down) with opposite spins.
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5
Q

What is the Liquid Drop model?

A

Based on observation that nearly all nuclei have same density, individual nucleons are analagous to molecules in a liquid held together by Van der Waals interactions and/or hydrogen binding and surface tension effects.

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6
Q

What is the first step in deriving an expression for binding energy of a nucleus?

A

Since nuclear forces show saturation there is a term proportional to A, i.e. C1*A, where C1 is extracted from experimental data.

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7
Q

What is the second step in deriving an expression for binding energy of a nucleus?

A

Nucleons on surface of a nucleus are less tightly bound than those in interior of nucleus…negative term, proportional to 4πR^2 -> -C2*A^2/3

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8
Q

What is the third step in deriving an expression for binding energy of a nucleus?

A

Each one of the protons repels the others. Electric interaction proportional to 1/R: term = -C3*z(z-1)/A^1/3

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9
Q

What is the fourth step in deriving an expression for binding energy of a nucleus?

A

From experiments, nuclei appear to need a balance between energies associated with neutrons and protons so that N~Z for small A and N slightly greater than Z for lare nuclei: -C4*(A-2Z)^2/A

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10
Q

What is the fifth step in deriving an expression for binding energy of a nucleus?

A

Nuclear force favours pairing of protons and neutrons. Positive term if Z and N are even, negative if both are odd, zero otherwise: +-C5*A^-4/3

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11
Q

What is, therefore, the equation for the binding energy of a nucleus?

A

E(B) = C1A-C2A^2/3 - C3z(z-1)/A^1/3 - C4(A-2Z)^2/A +-C5*A^-4/3

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12
Q

What s the equation for the mass of a neutral atom?

A

M = Z(m(p)-m(e))+Nm(n)-E(B)/c^2

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13
Q

What is the shell model of protons and neutrons in a nucleus?

A

For protons, there is an additional potential energy associated with the Coulomb repulsion -> each proton considered to interact with a sphere of uniform charge density of radius R and total charge (Z-1)e

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14
Q

What does the graph of V against r look like for the shell model of protons and neutrons?

A

Vcoulomb at top is curve curving down to x-axis, Vnuc is bottom curving up, so Vtot is combination of these so a bit higher than Vnuc.

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15
Q

What are the “magic numbers” of protons or neutrons? What does this mean?

A

2, 8, 20, 28, 50, 82, 126: these nuclei are very stable.

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16
Q

What number of protons must there be for the velocity of an electron not to exceed c?

A

Z < 137

17
Q

What is the heaviest nucleus found to be so far?

A

Z = 118, but naturally occurring: Uranium Z = 92

18
Q

What 2 eigenvalues does the spin operator s(zhat) have?

A

ћ/2, -ћ/2 for up and down spin respectively

19
Q

How do we work out the eigenvalues and eigenfunctions for s(zhat)?

A

Choose 2x2 matrix, so s(zhat) = ћ/2*matrix(1, 0, 0, -1), and then multiply this by matrix (a,b), where the 2x2 matrix = λ

20
Q

What do we do with the 2x2 matrix λ multiplied by matrix(a,b)?

A

Find values of a and b for λ = ћ/2 and λ = -ћ/2, find 2 eigenfunctions matrix(1,0) and matrix(0,1)

21
Q

What do we do after finding the eigenfunctions for s(zhat)?

A

Use s(zhat)X(sms) = m(s)ћ*X(sms)

22
Q

What do we find s(xhat) equals?

A

s(xhat) = ћ/2 *matrix(0, 1, 1, 0) = ћ/2 *σ(xhat)

23
Q

What do we find s(yhat) equals?

A

s(xhat) = ћ/2 *matrix(0, -i, i, 0) = ћ/2 *σ(yhat)

24
Q

What do we find s(zhat) equals?

A

s(xhat) = ћ/2 *matrix(1, 0, 0, -1) = ћ/2 *σ(zhat)

25
Q

What property of the spin matrices σ(xhat), σ(yhat) and σ(zhat) do we find?

A

σ(xhat)^2 = σ(yhat)^2 = σ(zhat)^2 = matrix(1, 0, 0, 1) = 1, and s(hat)^2 = s(xhat)^2 + s(yhat)^2 + s(zhat)^2 = 3ћ^2/2 *matrix(1, 0, 0, 1)

26
Q

What is the weak force responsible for?

A

Responsible for beta decay of some isotopes and nuclear fusion processes.

27
Q

What are the 4 fundamental particles in QM?

A

electrons, electron neutrinos, protons and neutrons.

28
Q

Which forces do quarks encounter?

A

strong, EM and weak

29
Q

Which forces do leptons encounter?

A

charged electrons, muons, tauons etc experience EM and weak but not strong, neutrinos experience only weak

30
Q

What are interactions in QFT mediated by?

A

Exchange of ‘virtual’ photons.

31
Q

What is a gauge boson?

A

Each of the 3 forces described by QFT corresponding to exchange of spin-1 force carrying particle known as a gauge boson.

32
Q

What is the gauge boson for the EM force?

A

The photon -> massless.

33
Q

What is the gauge boson for the strong force?

A

The gluon -> massless.

34
Q

What is the gauge boson for the weak force?

A

Mediated by charged W+ and W- bosons which are about 80 times more massive than protons.

35
Q

What are Feynman diagrams?

A

Used to describe some amplitude for a process on the way to summing over all appropriate processes to complete a calculation.

36
Q

What is one example of a Feynman diagram?

A

1 electron emits a photon γ which another electron absorbs. Interaction points are called g1, and g1 is proportional to charge, α proportional to g1^2, and measures the strength of the coupling.

37
Q

What is the equation for the dimensionless measure α?

A

α = e^2/4πε0ћc ~ 1/137

38
Q

What is another example of a Feynman diagram?

A

Muon decay: a muon emits W- and turns imto a muon neutrino. The W- boson decays into an electron and an anti-neutrino.

39
Q

What is the Higgs boson for?

A

Used to provide the mechanism by which all other particles acquire mass.