All 42 concepts.
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- 01 · Topology versus geometry
Geometry measures distances and angles; topology tracks properties unchanged by continuous deformation.Foundations of Topology - 02 · Open sets, continuity and compactness
Topology supplies a precise definition of continuity without first choosing a distance.Foundations of Topology - 03 · Connectedness and topological sectors
Disconnected regions of a configuration space cannot be connected by an allowed continuous path.Foundations of Topology - 04 · Homotopy and winding
A loop can wrap a circle an integer number of times; smooth deformations cannot change that integer without breaking continuity.Foundations of Topology - 05 · Manifolds, spheres and tori
A manifold looks locally like Euclidean space, even when its global topology is different.Foundations of Topology - 06 · Euler characteristic and genus
Counting vertices, edges and faces reveals a global invariant of a closed orientable surface.Foundations of Topology - 07 · Fiber bundles and quantum eigenstates
A quantum eigenstate can be defined locally while a single smooth global phase convention may fail to exist.Foundations of Topology - 08 · Gauge transformations and observables
The phase assigned to an eigenvector is conventional; measurable holonomy and curvature are not.Foundations of Topology - 09 · Projective Hilbert space
Two state vectors differing only by a nonzero complex factor represent the same pure quantum state.Geometric Quantum Mechanics - 10 · Berry phase and adiabatic evolution
A slowly transported eigenstate acquires a geometric phase in addition to its dynamical phase.Geometric Quantum Mechanics - 11 · Berry curvature as effective magnetic field
Berry curvature plays the role of a magnetic field in parameter or momentum space.Geometric Quantum Mechanics - 12 · Holonomy and Wilson loops
Parallel transport around a closed path can rotate a quantum state or a degenerate subspace.Geometric Quantum Mechanics - 13 · Aharonov–Bohm phase
A charged quantum wavefunction responds to enclosed magnetic flux even along paths with zero local magnetic field.Geometric Quantum Mechanics - 14 · Fubini–Study quantum metric
Quantum states have a natural notion of distance that measures how quickly distinguishable states change.Geometric Quantum Mechanics - 15 · Bloch theorem and Brillouin torus
Periodic lattices let us label electronic states by crystal momentum.Topological Band Theory - 16 · Chern number from Berry curvature
Integrating Berry curvature over a closed momentum-space surface yields an integer topological invariant.Topological Band Theory - 17 · TKNN quantization and Hall conductance
Hall conductivity can be locked to integers because it is the integral of band geometry.Topological Band Theory - 18 · Landau levels and integer quantum Hall effect
A perpendicular magnetic field organizes two-dimensional electron motion into quantized cyclotron levels.Topological Band Theory - 19 · Bulk–boundary correspondence
A change of bulk topology across an interface requires gap-crossing boundary states under suitable assumptions.Topological Band Theory - 20 · Haldane model and Chern insulators
Complex next-neighbor hopping can generate a quantum Hall-like phase without net magnetic flux per unit cell.Topological Band Theory - 21 · SSH model and winding number
A one-dimensional dimerized chain has distinct gapped winding sectors.Topological Band Theory - 22 · Zak phase and polarization
The Berry phase across a one-dimensional Brillouin zone is related to electric polarization.Topological Band Theory - 23 · Time-reversal symmetry and Z2 topology
Time-reversal symmetry can protect helical edge modes even when total Chern number vanishes.Topological Band Theory - 24 · Topological insulators in three dimensions
Three-dimensional time-reversal-invariant insulators can have robust surface Dirac states.Topological Band Theory - 25 · Weyl semimetals and monopoles
Weyl nodes act as sources or sinks of Berry curvature in three-dimensional momentum space.Topological Band Theory - 26 · Disorder and topological robustness
Topological properties can survive many imperfections because small perturbations cannot change a discrete invariant continuously.Topological Band Theory - 27 · Fractional quantum Hall effect
Strongly interacting electrons can form incompressible liquids with fractionally charged excitations.Interacting Topological Phases - 28 · Anyons and braid statistics
In two spatial dimensions, exchanges can have richer statistics than bosons or fermions.Interacting Topological Phases - 29 · Topological order and long-range entanglement
Some many-body phases cannot be characterized by local symmetry-breaking order parameters.Interacting Topological Phases - 30 · Toric code and stabilizers
Local commuting operators can produce a globally entangled ground space.Interacting Topological Phases - 31 · Majorana zero modes
A Majorana operator is its own Hermitian conjugate and can describe a zero-energy boundary mode in a superconducting model.Interacting Topological Phases - 32 · Kitaev chain and topological superconductivity
A simple one-dimensional p-wave superconducting model can host unpaired Majorana end modes.Interacting Topological Phases - 33 · Non-Abelian braiding and encoded gates
Exchanging non-Abelian anyons can rotate a protected degenerate subspace.Interacting Topological Phases - 34 · Symmetry-protected topological phases
Some short-range-entangled phases become distinct only when a symmetry is enforced.Interacting Topological Phases - 35 · Why topology emerges from quantum mechanics
Quantum superposition, phase, and interference make eigenstates vary continuously across parameter spaces; global patterns can then become topological.Quantum Phenomena and Applications - 36 · Gap closing and topological phase transitions
A topological index cannot change smoothly while its defining gap and symmetries remain intact.Quantum Phenomena and Applications - 37 · Topological photonics
Light propagating through engineered structures can inherit topological band features.Quantum Phenomena and Applications - 38 · Topological quantum sensing
Geometric phases and topological features can be used to encode or stabilize sensing signals.Quantum Phenomena and Applications - 39 · Cold atoms and synthetic dimensions
Laser-assisted hopping can simulate gauge fluxes and topological band structures with neutral atoms.Quantum Phenomena and Applications - 40 · Quantum computing with topological codes
Logical quantum information can be stored nonlocally in stabilizer-code degrees of freedom.Quantum Phenomena and Applications - 41 · Experimental diagnostics of topology
Different topological phases demand different experimental evidence.Quantum Phenomena and Applications - 42 · Topology, decoherence and limitations
Topological invariants can protect selected structures, but real quantum systems still couple to environments.Quantum Phenomena and Applications