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  2. Section (fiber bundle) - Wikipedia

    en.wikipedia.org/wiki/Section_(fiber_bundle)

    The (local) sections form a sheaf over called the sheaf of sections of . The space of continuous sections of a fiber bundle E {\displaystyle E} over U {\displaystyle U} is sometimes denoted C ( U , E ) {\displaystyle C(U,E)} , while the space of global sections of E {\displaystyle E} is often denoted Γ ( E ) {\displaystyle \Gamma (E)} or Γ ...

  3. Fiber bundle - Wikipedia

    en.wikipedia.org/wiki/Fiber_bundle

    A local section of a fiber bundle is a continuous map : where U is an open set in B and (()) = for all x in U. If ( U , φ ) {\displaystyle (U,\,\varphi )} is a local trivialization chart then local sections always exist over U .

  4. Cross section (geometry) - Wikipedia

    en.wikipedia.org/wiki/Cross_section_(geometry)

    For instance, while all the cross-sections of a ball are disks, [2] the cross-sections of a cube depend on how the cutting plane is related to the cube. If the cutting plane is perpendicular to a line joining the centers of two opposite faces of the cube, the cross-section will be a square, however, if the cutting plane is perpendicular to a ...

  5. Barn (unit) - Wikipedia

    en.wikipedia.org/wiki/Barn_(unit)

    As a simplified example, if a beamline runs for 8 hours (28 800 seconds) at an instantaneous luminosity of 300 × 10 30 cm −2 ⋅s −1 = 300 μb −1 ⋅s −1, then it will gather data totaling an integrated luminosity of 8 640 000 μb −1 = 8.64 pb −1 = 0.008 64 fb −1 during this period. If this is multiplied by the cross-section ...

  6. Principal bundle - Wikipedia

    en.wikipedia.org/wiki/Principal_bundle

    The local version of the cross section theorem then states that the equivariant local trivializations of a principal bundle are in one-to-one correspondence with local sections. Given an equivariant local trivialization ({U i}, {Φ i}) of P, we have local sections s i on each U i. On overlaps these must be related by the action of the structure ...

  7. Poincaré map - Wikipedia

    en.wikipedia.org/wiki/Poincaré_map

    A two-dimensional Poincaré section of the forced Duffing equation. In mathematics, particularly in dynamical systems, a first recurrence map or Poincaré map, named after Henri Poincaré, is the intersection of a periodic orbit in the state space of a continuous dynamical system with a certain lower-dimensional subspace, called the Poincaré section, transversal to the flow of the system.

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  9. Foliation - Wikipedia

    en.wikipedia.org/wiki/Foliation

    2-dimensional section of Reeb foliation 3-dimensional model of Reeb foliation. In mathematics (differential geometry), a foliation is an equivalence relation on an n-manifold, the equivalence classes being connected, injectively immersed submanifolds, all of the same dimension p, modeled on the decomposition of the real coordinate space R n into the cosets x + R p of the standardly embedded ...