Understanding the Basics
* Electric Quadrupole Moment: This quantity measures the deviation of a charge distribution from spherical symmetry. A positive quadrupole moment indicates a prolate (football-like) shape, while a negative moment indicates an oblate (pancake-like) shape.
* Extreme Single-Particle Model: This model simplifies the nucleus by assuming that all nucleons (protons and neutrons) except one are in a spherically symmetric core. The single particle outside the core contributes the entire quadrupole moment.
Calculation
1. Consider the Single Particle: We need to focus on the single particle outside the core. Let's assume it has a charge *e* and is in an orbital with angular momentum *l*.
2. Quantize the Angular Momentum: In quantum mechanics, the *z*-component of angular momentum is quantized, meaning it can only take on discrete values: *m*ħ, where *m* ranges from -*l* to +*l*.
3. Define the Quadrupole Moment Operator: The quadrupole moment operator, *Q*, is given by:
*Q* = (2/e) Σ *i* (3*zi2 - *ri2)
* *i* denotes each particle in the nucleus.
* *zi* is the *z*-coordinate of the *i*-th particle.
* *ri* is the radial distance of the *i*-th particle from the nucleus's center.
4. Evaluate for the Single Particle: Since we're dealing with the extreme single-particle model, we only need to consider the single particle's contribution:
*Q* = (2/e) (3*z2 - *r2)
5. Express in Spherical Coordinates: Convert *z* and *r* to spherical coordinates (r, θ, φ):
* *z* = *r* cos(θ)
* *r2* = *r2*
6. Simplify: Substitute into the quadrupole moment equation:
*Q* = (2/e) *r2 (3 cos2(θ) - 1)
7. Average over Angular Coordinates: The quadrupole moment is an expectation value. To find it, we need to average over all possible angles:
*Q* = (2/e) *r2 ∫02π dφ ∫0π sin(θ) (3 cos2(θ) - 1) dθ
8. Evaluate the Integrals: The integral evaluates to:
*Q* = (4/5) *e* *r2
9. Final Expression: The electric quadrupole moment for a single particle in the extreme single-particle model is:
*Q* = (4/5) *e* *r2
Interpretation
* The quadrupole moment depends on the charge (*e*) and the radial distance squared (*r2*) of the single particle.
* A larger *r* (particle farther from the core) leads to a larger quadrupole moment.
* The sign of the quadrupole moment (positive in this case) indicates a prolate shape, consistent with a single particle sitting outside a spherically symmetric core.
Note: This calculation assumes a single particle in the nucleus. For real nuclei, multiple particles contribute, and more sophisticated models are needed to accurately calculate the quadrupole moment.