OBSERVATION CHAMBER / ACTIVE

Berry Phase Holonomy Observatory

Carry a two-level eigenstate around closed loops on the Bloch sphere and compare its Berry phase with the enclosed curvature.

quantum / holonomy Observation Model

ROUTE 74 / GEOMETRY / QUANTUM HOLONOMY

TWO-LEVEL / BLOCH SPHERE

Carry one eigenstate around a closed loop

Move the direction of a two-level Hamiltonian on the Bloch sphere. Parallel transport leaves a gauge-invariant Berry phase that follows the oriented curvature.

READY

The sphere is Hamiltonian parameter space, not a measured physical trajectory. The wheel shows the selected band holonomy modulo 2π.

All calculations stay local in this browser.

Band
+
Loop
LATITUDE CAP
theta0
0.90 rad
Delta
1.00
Gap
2.00
Berry phase gamma
Solid angle Omega
Local Ftheta phi
Min overlap

GEOMETRIC READOUT

Phase from curvature

PASS
Berry phase gamma selected
Solid angle Omega
Curvature Ftheta phi
Energy gap g
Minimum overlap
Eigen residual
Phase residual
Trace progress
0 / 512
Interpretation
The displayed phase is geometric holonomy of an eigenline. It is not a dynamic phase and it is not a physical measurement.

For the stated eigenvector convention, gamma plus = −Omega/2 and gamma minus = +Omega/2 modulo 2 pi. The gap protects the two bands in this finite numerical model.

BANDGAMMACURVATUREPHASE RESIDUALEIGEN RESIDUAL

DETERMINISTIC SELF-TEST

Numerical acceptance

PASS

CAP / PASS

CHECKVALUELIMITRESULT
Observation report

OBSERVATION CONTRACT

One eigenline, one closed loop

The Hamiltonian direction n moves on the Bloch sphere. The selected eigenstate is parallel-transported along C, and the phase left after closure is the line-bundle holonomy. Dynamic time evolution is intentionally outside this chamber.

WHAT TO WATCH

Area, orientation, band

  • CAP grows the solid angle and the magnitude of gamma.
  • REVERSE changes the sign of the same geometric phase.
  • RETRACE cancels area; FIGURE 8 cancels opposite lobes while the local curvature remains visible.

MODEL NOTE

Finite two-level model

H = Delta n dot sigma, n = (sin theta cos phi, sin theta sin phi, cos theta)

F plus = −(sin theta / 2) dtheta wedge dphi, gamma plus = −Omega / 2. The lower band has the opposite signs.

This page observes a numerical eigenline bundle. It does not claim a laboratory measurement, a material property, or a visitor score.

Formula note

e^(i gamma) = product_j <u_j | u_(j+1)> / |<u_j | u_(j+1)>|. The implementation uses the negative argument of the overlap product because the transported vector removes each local overlap phase. The solid angle is computed independently from oriented spherical triangles.

OBSERVATION GUIDE

Touchpoints for observation

Start with CAP and the upper band. Press TRACE, then compare CAP with REVERSE and RETRACE. Lower Delta changes the gap only; changing the band reverses the curvature sign.

  • Use STEP to inspect the transported marker one segment at a time.
  • Use FIGURE 8 to see local curvature without a large net phase.
  • Use REPORT or PNG for the current screen. Reduced-motion keeps TRACE static and leaves STEP available.

This is a finite deterministic two-level numerical model. It excludes dynamic phase and physical measurement.

Runs inside the browser with no upload and no registration.

OBSERVATION POLICY

This observatory runs a deterministic two-level Hamiltonian model in your browser. Eigenstates, loops, calculations, reports, and images stay local. It does not measure visitors, devices, or physical matter.