Quark Rotation Groups for the Atomic f Shell

1993 ◽  
pp. 367-371
Author(s):  
B. R. Judd ◽  
G. M. S. Lister
Keyword(s):  
1984 ◽  
Vol 47 (1-3) ◽  
pp. 153-174
Author(s):  
Marc De Brabanter ◽  
Heinrich H. Zettl
Keyword(s):  

2021 ◽  
Author(s):  
Esa Järvenpää ◽  
Maarit Järvenpää ◽  
Ville Suomala ◽  
Meng Wu

Topology ◽  
1962 ◽  
Vol 1 (2) ◽  
pp. 121-124 ◽  
Author(s):  
Ioan James ◽  
Emery Thomas
Keyword(s):  

Author(s):  
D. Theo

By exploiting the well known spin representations of the orthogonal groups O(l), Morris [12] was able to give a unified construction of some of the projective representations of Weyl groups W(Φ) which had previously only been available by ad hoc means [5]. The principal purpose of the present paper is to give a corresponding construction for projective representations of the rotation subgroups W+(Φ) of Weyl groups. Thus we construct non-trivial central extensions of W+(Φ) via the well-known double coverings of the rotation groups SO(l). This adaptation allows us to give a unified way of obtaining the basic projective representations of W+(Φ) from those of W(Φ) determined in [12]. Hence our work is a development of the recent work of Morris, and is an extension of Schur's work on the alternative groups [15].


Mathematics ◽  
2019 ◽  
Vol 7 (10) ◽  
pp. 935 ◽  
Author(s):  
Simone Fiori

The present paper recalls a formulation of non-conservative system dynamics through the Lagrange–d’Alembert principle expressed through a generalized Euler–Poincaré form of the system equation on a Lie group. The paper illustrates applications of the generalized Euler–Poincaré equations on the rotation groups to a gyrostat satellite and a quadcopter drone. The numerical solution of the dynamical equations on the rotation groups is tackled via a generalized forward Euler method and an explicit Runge–Kutta integration method tailored to Lie groups.


1994 ◽  
Vol 5 (2) ◽  
pp. 221-226 ◽  
Author(s):  
S. Świerczkowski

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