6. Nuclear Properties From Shell Model Flashcards

1
Q

What are special about the magic numbers?

A

They are nuclei with a specific number of protons and neutrons that have a larger binding energy

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2
Q

Describe how the magic numbers arise

A

When there is a large energy gap between the grouped SOC states
- Levels are fully filled, so the next energy level has a large gap

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3
Q

Describe the notation for the spin and parity of the ground state

A

( n l_j ) ^K e.g. (1s_1/2)^2

where K is the number of nucleons

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4
Q

What is the value of m_j for a filled shell?

A

0 as the positive and negative m_j’s will cancel out

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5
Q

Which type of nuclei always have spin 0?

A

Any even Z and even N nucleus

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6
Q

Why do any even Z and even N nuclei have a total spin of 0?

A

Even though the shell is not full, the sub shells are filed in order which pair nucleons together to minimise m_j

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7
Q

How can we calculate the spin of an even-odd nuclei?

A

By looking at the total angular momentum of the shell where the unpaired nucleon is
- The spins of filled sub shells are 0

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8
Q

How do we calculate the spin of an odd-odd nucleus?

A

Given by the QM sum of the contribution of the unpaired protons and neutrons
- In the range of | j_p - j_n | to |j_p + j_n |

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9
Q

Define parity

A

The reflection of the spatial coordinates

r -> -r

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10
Q

State the effects of the parity operator acting on the spherical harmonics

A

P Y^m _l (theta, phi) = (-1)^l Y^m _l (theta, phi)

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11
Q

What is the intrinsic parity of a nucleon, and how can the parity be calculated for a multi-particle state?

A

Defined to be positive for a nucleon
- Only the parities of unpaired nucleons will determine the nucleus parity
P = product (-1)^l

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12
Q

What is the notation for the parity and ang. mom. of the nucleus

A

J^P

e.g. 5/2 ^ +

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13
Q

What are the two sources for a nucleus haveing a non-0 spin, and what is a consequence of this?

A

non-0 spin = non-0 magnetic dipole moment
Can be caused by:
1. Intrinsic magnetic moment of nucleons
2. Proton charge moving producing a magnetic moment

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14
Q

What is the equation for the nuclear magnetic moment?

A

μ = g_j * j * μ_N
g_j - Landé g factor
j - Nuclear spin
μ_N - Nuclear magneton

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15
Q

In which cases is the nuclear magnetic moment calculation most accurate?

A

For even-odd nuclei, where there is one unpaired nucleons

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16
Q

Between which two values do most nuclear magnetic moments lie?

A

Between j = l + 1/2 and j = l - 1/2

17
Q

Why doesn’t the nuclear magnetic moment calculation work well for odd-odd nuclei?

A

To calculate μ = g_j * j * μ_N, we need to calculate g_j which involves combining the spin component with the orbital component
- Would be harder when considering more the magnetic moments of more than one nucleon

18
Q

Define lowest excitation

A

The lowest excitation is the movement of the last unpaired nucleon to the next subshell
- Or moving a nucleon from the last filled subshell to the subshell with the remaining unapaired nucleon

19
Q

Which assumption leads to the limitation of the accuracy of the nuclear shell model?

A

That nucleons are moving freely, independent of other nucleons in a spherically symmetric potential