No Arabic abstract
We introduce the extended Freudenthal-Rosenfeld-Tits magic square based on six algebras: the reals $mathbb{R}$, complexes $mathbb{C}$, ternions $mathbb{T}$, quaternions $mathbb{H}$, sextonions $mathbb{S}$ and octonions $mathbb{O}$. The ternionic and sextonionic rows/columns of the magic square yield non-reductive Lie algebras, including $mathfrak{e}_{7scriptscriptstyle{frac{1}{2}}}$. It is demonstrated that the algebras of the extended magic square appear quite naturally as the symmetries of supergravity Lagrangians. The sextonionic row (for appropriate choices of real forms) gives the non-compact global symmetries of the Lagrangian for the $D=3$ maximal $mathcal{N}=16$, magic $mathcal{N}=4$ and magic non-supersymmetric theories, obtained by dimensionally reducing the $D=4$ parent theories on a circle, with the graviphoton left undualised. In particular, the extremal intermediate non-reductive Lie algebra $tilde{mathfrak{e}}_{7(7)scriptscriptstyle{frac{1}{2}}}$ (which is not a subalgebra of $mathfrak{e}_{8(8)}$) is the non-compact global symmetry algebra of $D=3$, $mathcal{N}=16$ supergravity as obtained by dimensionally reducing $D=4$, $mathcal{N}=8$ supergravity with $mathfrak{e}_{7(7)}$ symmetry on a circle. The ternionic row (for appropriate choices of real forms) gives the non-compact global symmetries of the Lagrangian for the $D=4$ maximal $mathcal{N}=8$, magic $mathcal{N}=2$ and magic non-supersymmetric theories obtained by dimensionally reducing the parent $D=5$ theories on a circle. In particular, the Kantor-Koecher-Tits intermediate non-reductive Lie algebra $mathfrak{e}_{6(6)scriptscriptstyle{frac{1}{4}}}$ is the non-compact global symmetry algebra of $D=4$, $mathcal{N}=8$ supergravity as obtained by dimensionally reducing $D=5$, $mathcal{N}=8$ supergravity with $mathfrak{e}_{6(6)}$ symmetry on a circle.
In this paper, we prove a new integral representation for the Bessel function of the first kind $J_mu(z)$, which holds for any $mu,zinmathbb{C}$.
A Fourier-type integral representation for Bessels function of the first kind and complex order is obtained by using the Gegenbuaer extension of Poissons integral representation for the Bessel function along with a trigonometric integral representation of Gegenbauers polynomials. This representation lets us express various functions related to the incomplete gamma function in series of Bessels functions. Neumann series of Bessel functions are also considered and a new closed-form integral representation for this class of series is given. The density function of this representation is simply the analytic function on the unit circle associated with the sequence of coefficients of the Neumann series. Examples of new closed-form integral representations of special functions are also presented.
It is shown that the quantum ground state energy of particle of mass m and electric charge e moving on a compact Riemann surface under the influence of a constant magnetic field of strength B is E_0=eB/2m. Remarkably, this formula is completely independent of both the geometry and topology of the Riemann surface. The formula is obtained by reinterpreting the quantum Hamiltonian as the second variation operator of an associated classical variational problem.
According to classical electrodynamics, sunlight that is passed through an iron layer can be detected with the naked eye only if the thickness of the layer is less than 170nm. However, in an old experiment, August Kundt was able to see the sunlight with the naked eye even when it had passed an iron layer with thickness greater than 200nm. To explain this observation, we propose a second kind of light which was introduced in a different context by Abdus Salam. A tabletop experiment can verify this possibility.
A simple model of the dynamics of lightly bound skyrmions is developed in which skyrmions are replaced by point particles, each carrying an internal orientation. The model accounts well for the static energy minimizers of baryon number $1leq Bleq 8$ obtained by numerical simulation of the full field theory. For $9leq Bleq 23$, a large number of static solutions of the point particle model are found, all closely resembling size $B$ subsets of a face centred cubic lattice, with the particle orientations dictated by a simple colouring rule. Rigid body quantization of these solutions is performed, and the spin and isospin of the corresponding ground states extracted. As part of the quantization scheme, an algorithm to compute the symmetry group of an oriented point cloud, and to determine its corresponding Finkelstein-Rubinstein constraints, is devised.