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Intersecting stacks of supersymmetric fractional branes on the Z_6' orientifold may be used to construct the supersymmetric Standard Model. If $a,b$ are the stacks that generate the SU(3)_{colour} and SU(2)_L gauge particles, then, in order…

高能物理 - 理论 · 物理学 2008-12-18 David Bailin , Alex Love

We construct N=1 supersymmetric fractional branes on the Z_6' orientifold. Intersecting stacks of such branes are needed to build a supersymmetric standard model. If a,b are the stacks that generate the SU(3)_c and SU(2)_L gauge particles,…

高能物理 - 理论 · 物理学 2016-09-06 David Bailin , Alex Love

We construct N=1 supersymmetric fractional branes on the Z_6' orientifold. Intersecting stacks of such branes are needed to build a supersymmetric standard model. If $a,b$ are the stacks that generate the SU(3)_c and SU(2)_L gauge…

高能物理 - 理论 · 物理学 2008-11-26 David Bailin , Alex Love

We construct N=1 supersymmetric fractional branes on the Z_6' orientifold. Intersecting stacks of such branes are needed to build a supersymmetric standard model. If a,b are the stacks that generate the SU(3)_c and SU(2)_L gauge particles,…

高能物理 - 理论 · 物理学 2008-11-26 David Bailin , Alex Love

In this paper, globally N=1 supersymmetric configurations of intersecting D6-branes on the Z6-orientifold are discussed, involving also fractional branes. It turns out rather miraculously that one is led almost automatically to just ONE…

高能物理 - 理论 · 物理学 2014-11-18 Gabriele Honecker , Tassilo Ott

We construct four dimensional three generation non-supersymmetric $SU(3)_c \times SU(2)_L \times U(1)_Y$ intersecting D6-brane models with $\nu_R$\rq{s}. At three stacks we find exactly the MSSM chiral fermion matter spectrum. At 4-,…

高能物理 - 理论 · 物理学 2014-02-19 Christos Kokorelis

We construct a new set of intersecting D4-brane models that yield the (non-supersymmetric) standard model up to vector-like matter and, in some cases, extra U(1) factors in the gauge group. The models are constrained by the requirement that…

高能物理 - 理论 · 物理学 2010-04-05 D. Bailin , G. V. Kraniotis , A. Love

We construct an N=1 supersymmetric three-family flipped SU(5) model from type IIA orientifolds on $T^6/(\Z_2\times \Z_2)$ with D6-branes intersecting at general angles. The spectrum contains a complete grand unified and electroweak Higgs…

高能物理 - 理论 · 物理学 2009-11-11 C. -M. Chen , G. V. Kraniotis , V. E. Mayes , D. V. Nanopoulos , J. W. Walker

We construct the first three family N=1 supersymmetric string model with Standard Model gauge group SU(3)_C x SU(2)_L x U(1)_Y from an orientifold of type IIA theory on T^6/(Z_2 x Z_2) and D6-branes intersecting at angles. In addition to…

高能物理 - 理论 · 物理学 2008-11-26 Mirjam Cvetic , Gary Shiu , Angel M. Uranga

We construct six stack D6-brane vacua (non-supersymmetric) that have at low energy exactly the standard model (with right handed neutrinos). The construction is based on D6-branes intersecting at angles in $D = 4$ type toroidal orientifolds…

高能物理 - 理论 · 物理学 2014-11-18 Christos Kokorelis

We construct new supersymmetric SU(5) Grand Unified Models based on Z4 x Z2 orientifolds with intersecting D6-branes. Unlike constructions based on Z2 x Z2 orientifolds, the orbifold images of the three-cycles wrapped by D6-branes…

高能物理 - 理论 · 物理学 2008-11-26 Mirjam Cvetic , Paul Langacker

We construct supersymmetric composite models of quarks and leptons from type IIA T^6/(Z_2 x Z_2) orientifolds with intersecting D6-branes. In case of T^6 = T^2 x T^2 x T^2 with no tilted T^2, a composite model of the supersymmetric SU(5)…

高能物理 - 理论 · 物理学 2009-11-10 Noriaki Kitazawa

By introducing an extra stack of D6-branes to standard ${\cal N}=1$ supersymmetric Pati-Salam models, we extend the landscape of its complete search. In this construction, the $d$-stack of D6-branes is introduced besides the standard…

高能物理 - 理论 · 物理学 2026-01-09 Haotian Huangfu , Tianjun Li , Qi Sun , Rui Sun

I describe the main features of new intersecting D4- and D5-brane orbifold models that yield the non-supersymmetric standard model, up to vector-like matter and, in some cases, extra U(1) factors in the gauge group. There are six-stack…

高能物理 - 理论 · 物理学 2009-11-07 D. Bailin

We construct new D6-brane model vacua (non-supersymmetric) that have at low energy exactly the standard model spectrum (with right handed neutrinos). The minimal version of these models requires five stacks of branes. and the construction…

高能物理 - 理论 · 物理学 2009-11-07 Christos Kokorelis

We provide a systematic construction of three-family N=1 supersymmetric Pati-Salam models from Type IIA orientifolds on $\IT^6/(\IZ_2\times \IZ_2)$ with intersecting D6-branes. All the gauge symmetry factors $SU(4)_C\times SU(2)_L \times…

高能物理 - 理论 · 物理学 2009-09-17 Mirjam Cvetic , Tianjun Li , Tao Liu

Following the scanning methods of arXiv:1910.04530, we for the first time systematically construct the $N=1$ supersymmetric $SU(12)_C\times SU(2)_L\times SU(2)_R$ models, $SU(4)_C\times SU(6)_L\times SU(2)_R$ models, and $SU(4)_C\times…

高能物理 - 理论 · 物理学 2023-04-28 Tianjun Li , Adeel Mansha , Rui Sun

Employing new scanning methods, we revisit the systematic construction of three-family $N=1$ supersymmetric Pati-Salam models in Type IIA orientifolds on ${\bf T}^6/(\mathbb Z_2\times \mathbb Z_2)$ with intersecting D6-branes. Arising from…

高能物理 - 理论 · 物理学 2020-06-23 Tianjun Li , Adeel Mansha , Rui Sun

Using previous results on the statistics of intersecting D6-brane models on T^6/Z_6' we analyse solutions that resemble the gauge group and matter content of the supersymmetric standard model. In particular the structure of the hidden…

高能物理 - 理论 · 物理学 2008-11-26 Florian Gmeiner , Gabriele Honecker

We construct an N=1 supersymmetric three-family flipped SU(5) model from type IIA orientifolds on $T^6/(\Z_2\times \Z_2)$ with D6-branes intersecting at general angles. The model is constrained by the requirement that Ramond-Ramond tadpoles…

高能物理 - 理论 · 物理学 2009-11-11 C. -M. Chen , G. V. Kraniotis , V. E. Mayes , D. V. Nanopoulos , J. W. Walker
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