scholarly journals Phase structure of non-commutative field theories and spinning brane bound states

2000 ◽  
Vol 2000 (03) ◽  
pp. 024-024 ◽  
Author(s):  
Troels Harmark ◽  
Niels A Obers
2003 ◽  
Vol 668 (1-2) ◽  
pp. 293-321 ◽  
Author(s):  
Luis Álvarez-Gaumé ◽  
Miguel A. Vázquez-Mozo

2002 ◽  
pp. 1168-1169
Author(s):  
G. ARCIONI ◽  
J.L.F. BARBÓN ◽  
JOAQUIM GOMIS ◽  
M.A. VÁZQUEZ-MOZO

2003 ◽  
Vol 664 (1-2) ◽  
pp. 371-399 ◽  
Author(s):  
C. Becchi ◽  
S. Giusto ◽  
C. Imbimbo

2004 ◽  
Vol 2004 (05) ◽  
pp. 047-047 ◽  
Author(s):  
Wolfgang Bietenholz ◽  
Frank Hofheinz ◽  
Jun Nishimura

2011 ◽  
Vol 26 (06) ◽  
pp. 935-945 ◽  
Author(s):  
O. W. GREENBERG

We describe a method of solving quantum field theories using operator techniques based on the expansion of interacting fields in terms of asymptotic fields. For bound states, we introduce an asymptotic field for each (stable) bound state. We choose the nonrelativistic hydrogen atom as an example to illustrate the method. Future work will apply this N-quantum approach to relativistic theories that include bound states in motion.


1993 ◽  
Vol 08 (09) ◽  
pp. 1613-1628
Author(s):  
T. JAROSZEWICZ ◽  
P.S. KURZEPA

We derive and solve — in an arbitrary number of dimensions — Omnès-type equations for bound-state energies in weakly coupled quantum field theories. We show that, for theories defined in the 1/N expansion, these equations are exact to leading order in 1/N. We derive and discuss the weak coupling and nonrelativistic limits of the Omnès equations. We then calculate the binding energies and effective bound-state couplings in (1+1), (1+2) and (1+3)-dimensional O(N)-invariant ϕ4 theory. We consider both the scalar and symmetric tensor bound states.


1995 ◽  
Vol 10 (05) ◽  
pp. 739-751 ◽  
Author(s):  
ANDREAS FRING ◽  
ROLAND KÖBERLE

We demonstrate that the generalization of the Coleman–Thun mechanism may be applied to the situation where one considers scattering processes in 1 + 1 dimensions in the presence of reflecting boundaries. For affine Toda field theories we find that the binding energies of the bound states are always half the sum over a set of masses having the same color with respect to the bicoloration of the Dynkin diagram. For the case of E6 affine Toda field theory we compute explicitly the spectrum of all higher boundary bound states. The complete set of states constitutes a closed bootstrap.


Sign in / Sign up

Export Citation Format

Share Document