For an arbitrary solution of the system (2a)(2b), we perform two steps of Bäcklund transformations corresponding to distinct parameters k 1 and k 2 in different ...

A fermionic extension of K(- 1 , - 2) equation, alias a super K(- 1 , - 2) equation, proposed by Tempesta et al. (2003), is converted to the N = 1 ...

Hence, the system (2a)(2b) serves as a fermionic extension of K ( − 1 , − 2 ) equation, and would be also referred to as a super K ( − 1 , − 2 ) equation in ...

A fermionic extension of K(−1,−2) equation, alias a super K(−1,−2) equation, proposed by Tempesta et al. (2003), is converted to the N=1 supersymmetric ...

Majorana equation · 1 Definition. 1.1 Purely real four-component form · 2 Key ideas · 3 Two-component Majorana equation. 3.1 Weyl equation · 4 Four-component ...

= ζ(3/2) + Li3/2 e−µ0H/kBTc + Li3/2 e−2µ0H/kBTc . This is a transcendental equation for T = Tc(n, H). In the limit µ0H ≫ kBTc, the second two terms become.

Mar 16, 2022 · The NUT-parameter or the so-called NUT charge [2] was one of the two remaining parameters, which was eliminated from his solution because Kerr.

Jul 15, 2013 · Also, we substitute c=1/2 for a single real fermion, thus getting −1/48 at various places. The operator (−1)F is what switches the sign of ...

We now introduce reciprocal transformations for super equations (1) and (2), and connect them with two well-known super extensions of the KdV equation.

Electron Magnetism: The conduction electrons in a metal can be treated as a gas of fermions of spin 1/2 (with up/down degeneracy), and density n = N/V . (a) ...