Skip to content

Reading Spin and Geometric-Phase Diagrams

These diagrams show three different objects: a qubit state, angular wavefunction shapes, and interfering physical paths. Read the plotted object first; similar-looking arrows and lobes need not have the same meaning.

Bloch Coordinates, Angular Functions, and Physical Paths

Section titled “Bloch Coordinates, Angular Functions, and Physical Paths”

Bloch sphere with two-level state coordinates

Bloch-sphere coordinates for a normalized two-level state. The pole labels ∣1⟩,∣2⟩|1\rangle,|2\rangle identify the chosen basis, and rz=P(1)−P(2)r_z=P(1)-P(2). For a spin qubit ⟨S⟩=(ℏ/2)r\langle\mathbf S\rangle=(\hbar/2)\mathbf r. Pure states lie on the sphere and mixed states inside it; this is state geometry, not a particle trajectory. See Bloch Sphere.

Spherical harmonics angular shapes for low angular momenta

Schematic angular shapes: Y00Y_0^0, Y10Y_1^0, and the real combination Y1x=(Y1−1−Y11)/2∝sin⁡θcos⁡ϕY_{1x}=(Y_1^{-1}-Y_1^1)/\sqrt2\propto\sin\theta\cos\phi. Different gray fills distinguish opposite amplitude signs, not different probabilities. The drawn ellipses are shape mnemonics, not quantitative radial plots. The real Y1xY_{1x} is not an LzL_z eigenfunction. See Spherical Harmonics Quick Reference.

Two paths around an excluded magnetic flux region acquire an Aharonov–Bohm phase difference

Two paths enclosing excluded magnetic flux acquire a relative Aharonov–Bohm phase. The visual emphasizes holonomy in the accessible region, not a local force along the paths. See Aharonov–Bohm Effect.

For the Bloch diagram, an equatorial state has rz=0r_z=0, so P(1)=P(2)=1/2P(1)=P(2)=1/2. Moving around the equator changes their relative phase and changes measurements in other bases, even though those two populations stay fixed.

For the Aharonov–Bohm diagram, the loop follows one path forward and the other backward. Its orientation fixes the sign of the enclosed flux. The relative phase factor returns to itself when the flux changes by h/∣q∣h/|q| for charge q≠0q\ne0. A nonzero flux can therefore produce a trivial phase factor when it is an integer number of flux quanta. See the worked Berry Phase Problems for this distinction.

  • J. J. Sakurai and J. Napolitano, Modern Quantum Mechanics, 3rd ed., Cambridge University Press, 2020.
  • A. Shapere and F. Wilczek, eds., Geometric Phases in Physics, World Scientific, 1989.
  • E. Tufte, The Visual Display of Quantitative Information, 2nd ed., Graphics Press, 2001.
  • R. N. Zare, Angular Momentum: Understanding Spatial Aspects in Chemistry and Physics, Wiley, 1988.