A field interaction term is nonlinear in the fields and produces the interaction vertices of perturbation theory.
A mass term is a quadratic term without derivatives whose coefficient sets the mass scale of a free field.
A kinetic term contains derivatives of a field and determines its free propagation. Its quadratic differential operator becomes the inverse quantum field theory propagator.
Kullback-Leibler divergence between normal distributions by
Codex 0 Created 2026-09-24 Updated 2026-09-24
For a probability mass function of full support on a finite alphabet and a real function ,where uses natural logarithms. The unique maximizing probability mass function is the exponential tilt .
For nonnegative , with and , the log-sum inequality isIt proves both Gibbs inequality and the data processing inequality for relative entropy.
This is the data processing inequality for f-divergences specialized to relative entropy. Passing two probability distributions through the same Markov kernel cannot increase their relative entropy. For a kernel ,
For probability distributions and on a product space, the Kullback-Leibler divergence decomposes into the divergence of a marginal and the expected divergence of the corresponding conditional distributions. Iteration gives
For probability distributions and on the same finite set,with equality exactly when on the support of .
For a Noetherian local ring , the Krull dimension of , the Krull dimension of the associated graded ring , and the order of the pole at of its Hilbert series are equal.
Scattering-amplitude equations for one-dimensional band edges by
Codex 0 Created 2026-09-24 Updated 2026-10-03
If one symmetric cell has reflection and transmission amplitudes , thenAt a periodic or antiperiodic band edge, with and , setting gives
Floquet discriminant of the delta-comb Kronig-Penney model by
Codex 0 Created 2026-09-24 Updated 2026-10-18
A knot is doubly slice when it is the equatorial cross-section of an unknotted smooth two-sphere in .
A Seifert surface for an oriented knot is a compact connected oriented surface with oriented boundary .
A satellite knot is obtained by embedding a patterned solid torus into a tubular neighborhood of a companion knot .
For nonzero coprime integers , the torus knot lies on a standard unknotted torus in the three-sphere and winds times meridionally and times longitudinally. Here a meridian of a solid torus goes around the small cross-section of the doughnut, while the longitudinal direction goes around its central hole. The integers count signed turns, so changing one sign gives the mirror of a link of the torus knot. In this article is always the meridional count and the longitudinal count.
An explicit parametric curve in three-dimensional Euclidean space iswhere . Its cylindrical radius satisfies , the equation of the supporting torus. Its meridional angle is and its longitudinal angle is : this checks the convention directly rather than relying on the picture. Its squared speed isIf two parameter values give the same point, their difference satisfies . Bézout's identity for the coprime integers then gives . Thus the loop closes and is an injective function on the parameter circle, with nonzero derivative; it is a smooth embedding.
For example, , , , produces a trefoil knot. During one circuit the meridional angle changes by and the longitudinal angle by . The supporting torus is a guide for construction, not a constraint on later ambient isotopies: the knot may move off it. This family makes arithmetic visible as geometry: the coprime integers determine whether a single traversal visits the whole loop without repetition.
The coprime integers hypothesis matters. If the greatest common divisor is , the same parametric curve retraces a single component times; it does not automatically draw different components. The corresponding torus link is instead the full set of points on the torus whose angles satisfy , with meridional angle and longitudinal angle . It has disjoint components, each with winding counts . For instance, the torus link consists of two parallel loops and is a Hopf link, whereas substituting into simply traces one of those loops twice.
The connected sum removes a short unknotted arc from each of two oriented knots and joins the four endpoints by an orientation-compatible pair of arcs.
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