1987
DOI: 10.1007/bf01556168
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Grand unified theories in coset space dimensional reduction

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Cited by 14 publications
(4 citation statements)
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“…The embedding of R into G = G1 × G2 for the coset space (iii). (6), SO (10), G1 = SU (7), SO (12), SO (11), Sp( 10) SO( 13), Sp (12), E6 G2 = G2, Sp(4) G2 = SU(2) SU(5) × U(1) G1 = SU (6), SO (10), G1 = SU (7), SO( 13) SO (11), Sp( 10) Sp( 12), E6 G2 = G2, Sp(4) G2 = SU( 2) SO(10) × U(1) G1 = SO (12), SO( 13), G1 = SO (14), SO (15), E6 E7 G2 = G2, Sp(4)…”
Section: Table IVmentioning
confidence: 99%
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“…The embedding of R into G = G1 × G2 for the coset space (iii). (6), SO (10), G1 = SU (7), SO (12), SO (11), Sp( 10) SO( 13), Sp (12), E6 G2 = G2, Sp(4) G2 = SU(2) SU(5) × U(1) G1 = SU (6), SO (10), G1 = SU (7), SO( 13) SO (11), Sp( 10) Sp( 12), E6 G2 = G2, Sp(4) G2 = SU( 2) SO(10) × U(1) G1 = SO (12), SO( 13), G1 = SO (14), SO (15), E6 E7 G2 = G2, Sp(4)…”
Section: Table IVmentioning
confidence: 99%
“…Thus CSDR models of D = 10 can bridge the superstring theory and the SM. In this spirit, many works have been done in ten dimension, but no realistic model has emerged yet [3,12,13,14,15,16,17,18,19]. A major obstacle to build realistic models is the difficulty to obtain all the SM fermions.…”
Section: Introductionmentioning
confidence: 99%
“…One can obtain a chiral theory in four dimensions after the dimensional reduction even if one chooses that vector-like fermions present in these dimensions. However, no phenomenologically promising models have been found in D = 6, 10, 14 dimensions [26,[28][29][30][31][32][33][34].…”
Section: Introductionmentioning
confidence: 99%
“…This advantage increases the chance for the higher-dimensional model to be a promising candidate. No theories have been found quite promising, however, for the 6, 10, and 14 dimensional spacetimes [22,26,29,30,31,32,33,34,35,36].…”
Section: Introductionmentioning
confidence: 99%