Coherent electron flavor probability
Mint: numerical matter evolution. Dashed: the same entrance state propagated in vacuum. Gold marker: resonance crossing, when present. This is a calculation, not repeated measurements of a travelling particle.
Neutrinos · D07 · A changing quantum compass
Send one coherent neutrino state through a changing electron density. Follow its path on the Bloch sphere, compare vacuum evolution, and discover when slow conversion breaks down.
ONE STATE · A CHANGING MEDIUM
Mint: numerical matter evolution. Dashed: the same entrance state propagated in vacuum. Gold marker: resonance crossing, when present. This is a calculation, not repeated measurements of a travelling particle.
The horizontal axis is distance through an illustrative one-dimensional profile. It is not solar radius or a measured Earth model.
Gold: upper branch population. Rose: local mixing strength. Constant branch population indicates following in an instantaneous basis; it need not imply constant flavor.
Instantly set the potential to zero at exit, project onto vacuum mass states, then average away their relative phase. This average is a separate operation; it is not the coherent endpoint probability.
Exact unitary exponentials at interval midpoints. Compare 4,800 with 9,600 steps at 1,201 common positions. The difference diagnoses convergence; it is not an error guarantee. CSV retains all 9,601 positions. Dense chart columns show the sampled minimum and maximum within each pixel.
Electron flavor is the north pole; the other active flavor is the south pole. Bloch coordinates encode amplitudes, not real-space directions. Gold is the normalized trace-free Hamiltonian axis. The two-flavor splitting is positive. Antineutrinos reverse the charged-current potential; this real two-flavor model has no CP phase. Entrance eigenstates are recomputed when the medium changes. Vacuum comparisons always use the identical prepared entrance state.
Density means mass density times electrons per nucleon. The decreasing profile follows a shifted exponential over four decades and reaches zero exactly at exit. Solar-like means the shape and illustrative parameters, not a solar density fit. Constant density is abruptly removed at exit; its adiabatic vacuum-exit reference is inapplicable. No absorption or detector sampling is modeled.
CONTINUE EXPLORING
Propagation predicts a flavor probability. Which parts of the experiment turn an interaction into a usable record?
Physics tutorial
BackgroundCoherent forward scattering adds an electron-flavor potential. A density gradient rotates the instantaneous Hamiltonian axis; the quantum state may follow it or fail to keep up.
Why it mattersThis mechanism connects solar flavor conversion with matter effects in Earth. Here a prescribed two-flavor profile isolates that mechanism before any detector or realistic density model.
Start with the essentials
The flavor basis is electron, then other active. A common trace phase is removed. Distance uses kilometres, energy eV internally and the positive mass-squared splitting eV squared.
Density is mass density times electrons per nucleon. The potential changes sign for antineutrinos. Common active-flavor neutral-current terms do not change this two-flavor evolution.
For positive splitting and angles below 45 degrees, the positive-density resonance occurs for neutrinos. The gold axis is then transverse to the flavor axis. At zero mixing the exact level crossing has no off-diagonal conversion.
Project the exiting state onto vacuum mass states and discard their relative phase. This is not the coherent electron probability at the last position. The separate adiabatic reference assumes slow following all the way to a vacuum exit.
Typical misconceptionThe neutrino physically spirals around a sphere inside the Sun.
Better mental modelThe sphere encodes a normalized two-component quantum state. Its coordinates are amplitude coherences and flavor imbalance, not spatial coordinates.
Typical misconceptionElectron neutrinos disappear because matter blocks them.
Better mental modelThis Hermitian model conserves total active probability. The medium changes coherent evolution; no absorption is included.
Use Solar-like gradient and replay. Scrub across the gold resonance marker.
What to observe: The gold evolution axis rotates as density decreases. The state remains normalized while its electron probability changes.Compare Slow crossing and Sudden crossing. Both prepare the same upper entrance eigenstate and the same density range.
What to observe: A longer length makes the same density change slower per kilometre. The slow case nearly preserves the upper branch; the sudden case does not.Choose Constant resonance. Inspect the probability and branch curves.
What to observe: The local mixing is almost maximal; coherent flavor oscillations persist. The upper branch population is constant because the Hamiltonian is constant. The abrupt exit invalidates the slow-exit reference.Return to Solar-like gradient, select Antineutrino, then Propagate.
What to observe: For the positive splitting and angle used here, the positive-density resonance disappears. This two-flavor model has no CP phase; a matter-induced difference is not CP discovery.Inspect normalization and refinement diagnostics, then export the entire trajectory.
What to observe: Per-step unitarity protects normalization; density discretization can still change the trajectory. The step comparison diagnoses one numerical approximation, not all omitted physics.