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 supersymmetric Korteweg–de Vries equation via invertible transformations involving both independent and dependent variables.
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 ...
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 ...
Mar 15, 2022 · Kai Tian , Hanyu Zhou: On a fermionic extension of K(-1, -2) equation. Commun. Nonlinear Sci. Numer. Simul. 108: 106237 (2022).
May 1, 2022 · A fermionic extension of K ( − 1 , − 2 ) equation is changed to the N = 1 SUSY KdV equation. • A Bäcklund transformation and a nonlinear ...
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 ...
On a fermionic extension of K(−1,−2) equation. #18. Kai Tian. ,. Hanyu Zhou. (May, 2022). Published in: Commun.Nonlinear Sci.Numer.Simul. 108 (2022) 106237.
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 ...
hν with ν 2 Z. How can this be? Let us start with the first question. We have to make the distinction between two cases. (i) ...