Classification of closed-fermionic-string models

1986 ◽  
Vol 34 (12) ◽  
pp. 3794-3804 ◽  
Author(s):  
H. Kawai ◽  
D. C. Lewellen ◽  
S. -H. H. Tye
1989 ◽  
Vol 04 (24) ◽  
pp. 2339-2347 ◽  
Author(s):  
DAVID C. DUNBAR

It is shown that ZN orbifold models may, in special case be realised by a set world sheet fermions which have boundary conditions which are non-diagonal.


1987 ◽  
Vol 288 ◽  
pp. 1-76 ◽  
Author(s):  
Hikaru Kawai ◽  
David C. Lewellen ◽  
S.-H. Henry Tye

1986 ◽  
Vol 57 (15) ◽  
pp. 1832-1835 ◽  
Author(s):  
Hikaru Kawai ◽  
David C. Lewellen ◽  
S. -H. Henry Tye

1988 ◽  
Vol 03 (01) ◽  
pp. 279-284 ◽  
Author(s):  
HIKARU KAWAI ◽  
DAVID C. LEWELLEN ◽  
S.-H. HENRY TYE

The spin structure construction of four-dimensional fermionic string models of the heterotic type is extended by considering a generalized form of the world-sheet super-current. The rules for model building are given and illustrated with two sets of examples: the original spin structure construction and the Z3 asymmetric orbifold.


1987 ◽  
Vol 58 (4) ◽  
pp. 429-429 ◽  
Author(s):  
Hikaru Kawai ◽  
David C. Lewellen ◽  
S. -H. Henry Tye

2001 ◽  
Vol 16 (03) ◽  
pp. 425-482 ◽  
Author(s):  
G. B. CLEAVER ◽  
A. E. FARAGGI ◽  
D. V. NANOPOULOS

Three family SU (3)C× SU (2)L× U (1)Y string models in several constructions generically possess two features: (i) an extra local anomalous U (1)A and (ii) numerous (often fractionally charged) exotic particles beyond those in the minimal supersymmetric model (MSSM). Recently, we demonstrated that the observable sector effective field theory of such a free fermionic string model can reduce to that of the MSSM, with the standard observable gauge group being just SU (3)C× SU (2)L× U (1)Y and the SU (3)C× SU (2)L× U (1)Y-charged spectrum of the observable sector consisting solely of the MSSM spectrum. An example of a model with this property was shown. We continue our investigation of this model by presenting a large set of different flat directions of the same model that all produce the MSSM spectrum. Our results suggest that even after imposing the conditions for the decoupling of exotic states, there may remain sufficient freedom to satisfy the remaining phenomenological constraints imposed by the observed data.


1996 ◽  
Vol 11 (19) ◽  
pp. 3439-3477 ◽  
Author(s):  
JORGE L. LOPEZ ◽  
D.V. NANOPOULOS

We explore the postulates of string no-scale supergravity in the context of free-fermionic string models. The requirements of vanishing vacuum energy, flat directions of the scalar potential, and stable no-scale mechanism impose strong restrictions on possible string no-scale models, which must possess only two or three moduli, and a constrained massless spectrum. The soft-supersymmetry-breaking parameters involving all twisted and untwisted fields are given explicitly. Our calculations take into account the possible existence of an anomalous U A(1) factor in the gauge group, and reveal some novel effects concerning the stability of the no-scale mechanism in the presence of U A(1). This class of models contains no free parameters, i.e. in principle all supersymmetric particle masses and interactions are completely determined. A computerized search for free-fermionic models with the desired properties yields a candidate SU (5)×U(1) model containing extra [Formula: see text] matter representations that allow gauge coupling unification at the string scale. Our candidate model possesses a benign nonuniversal assignment of supersymmetry-breaking scalar masses, which may have interesting low-energy experimental consequences.


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