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When the hurlyburly’s done, When the battle’s lost and won.

When the hurlyburly’s done, When the battle’s lost and won. Minimize

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The Pennsylvania State University CiteSeerX Archives

Year of Publication:

2012-06-21

Source:

http://edoc.ub.uni-muenchen.de/8861/1/Akerblom_Nikolas.pdf

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xi

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Explicit formulas for the scalar modes in Seiberg-Witten theory with an application to the Argyres-Douglas point,” JHEP 0502

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Abstract: General formulas for the scalar modes ai and ai D in the Seiberg–Witten SU(N) setting are derived in the cases with and without massive hypermultiplets. Subsequently these formulas are applied in a study of the SU(3) Argyres–Douglas point. We use this example to study the question, whether the scalar modes admit an interpretation in te...

Abstract: General formulas for the scalar modes ai and ai D in the Seiberg–Witten SU(N) setting are derived in the cases with and without massive hypermultiplets. Subsequently these formulas are applied in a study of the SU(3) Argyres–Douglas point. We use this example to study the question, whether the scalar modes admit an interpretation in terms of BPS mass states everywhere in moduli space. The paper collects, in an appendix, various, which naturally appears in the derived formulas. facts on the function Lauricella F (n) D Minimize

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Year of Publication:

2013-01-30

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http://arxiv.org/pdf/hep-th/0409253v1.pdf

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dgf ; set ; sud. On leave of absence from ITP

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Explicit formulas for the scalar modes in Seiberg-Witten theory with an application to the Argyres-Douglas point,” JHEP 0502

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Abstract: General formulas for the scalar modes ai and ai D in the Seiberg–Witten SU(N) setting are derived in the cases with and without massive hypermultiplets. Subsequently these formulas are applied in a study of the SU(3) Argyres–Douglas point. We use this example to study the question, whether the scalar modes admit an interpretation in te...

Abstract: General formulas for the scalar modes ai and ai D in the Seiberg–Witten SU(N) setting are derived in the cases with and without massive hypermultiplets. Subsequently these formulas are applied in a study of the SU(3) Argyres–Douglas point. We use this example to study the question, whether the scalar modes admit an interpretation in terms of BPS mass states everywhere in moduli space. The paper collects, in an appendix, various, which naturally appears in the derived formulas. facts on the function Lauricella F (n) D Minimize

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The Pennsylvania State University CiteSeerX Archives

Year of Publication:

2012-04-02

Source:

http://www.itp.uni-hannover.de/~flohr/papers/sw-lauricella.pdf

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text

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en

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dgf ; set ; sud. On leave of absence from ITP

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Germany Explicit Formulas for the Scalar Modes in Seiberg–Witten TheoryExplicit Formulas for the Scalar Modes in Seiberg–Witten Theory

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why. I have attempted to deliver them in a spirit that should be recommended to all students embarking on writing their PhD theses: imagine that you are explaining your ideas to a former smart, but ignorant, self at the beginning of your studies!

why. I have attempted to deliver them in a spirit that should be recommended to all students embarking on writing their PhD theses: imagine that you are explaining your ideas to a former smart, but ignorant, self at the beginning of your studies! Minimize

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The Pennsylvania State University CiteSeerX Archives

Year of Publication:

2012-04-02

Source:

http://www.itp.uni-hannover.de/~flohr/papers/nikolas-thesis.pdf

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MPP-2007-55 LMU-ASC 30/07 Thresholds for Intersecting D-branes Revisited

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Gauge threshold corrections for intersecting D6-brane string models on toroidal orbifold backgrounds are reconsidered. Both by dimensionally regularising the appearing open string one-loop diagrams in tree-channel as well as by zeta-function regularisation of the corresponding loop-channel one-loop diagrams, we arrive at a result which takes int...

Gauge threshold corrections for intersecting D6-brane string models on toroidal orbifold backgrounds are reconsidered. Both by dimensionally regularising the appearing open string one-loop diagrams in tree-channel as well as by zeta-function regularisation of the corresponding loop-channel one-loop diagrams, we arrive at a result which takes into account the infrared divergence from the contribution of the massless states in the running of the gauge coupling constant as well as the contribution of states, which become light in certain regions of the moduli space. Contents Minimize

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The Pennsylvania State University CiteSeerX Archives

Year of Publication:

2012-11-22

Source:

http://arxiv.org/pdf/0705.2150v1.pdf

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en

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A Loop channel calculation and zeta-function regularisation 10

A Loop channel calculation and zeta-function regularisation 10 Minimize

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D-brane Instantons in 4D Supersymmetric String Vacua

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We review some aspects of D-instantons in intersecting D-brane models. In particular, we present applications of the recently proposed instanton calculus to computations of charged matter superpotential couplings and corrections to the gauge kinetic function in the low energy effective action of type IIA orientifolds. As an interesting byway, we...

We review some aspects of D-instantons in intersecting D-brane models. In particular, we present applications of the recently proposed instanton calculus to computations of charged matter superpotential couplings and corrections to the gauge kinetic function in the low energy effective action of type IIA orientifolds. As an interesting byway, we also discuss how one-loop corrections to the gauge kinetic function can be deduced from gauge threshold corrections in the type IIA setting. Minimize

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Year of Publication:

2013-09-30

Source:

http://arxiv.org/pdf/0712.1793v1.pdf

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Instantons and Holomorphic Couplings in Intersecting D-brane Models

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We clarify certain aspects and discuss extensions of the recently introduced string D-instanton calculus (hep-th/0609191). The one-loop determinants are related to one-loop open string threshold corrections in intersecting D6brane models. Utilising a non-renormalisation theorem for the holomorphic Wilsonian gauge kinetic functions, we derive a n...

We clarify certain aspects and discuss extensions of the recently introduced string D-instanton calculus (hep-th/0609191). The one-loop determinants are related to one-loop open string threshold corrections in intersecting D6brane models. Utilising a non-renormalisation theorem for the holomorphic Wilsonian gauge kinetic functions, we derive a number of constraints for the moduli dependence of the matter field Kähler potentials of intersecting D6-brane models on the torus. Moreover, we compute string one-loop corrections to the Fayet-Iliopoulos terms on the D6-branes finding that they are proportional to the gauge threshold corrections. Employing these results, we discuss the issue of holomorphy for E2-instanton corrections to the superpotential. Eventually, we discuss E2-instanton corrections to the gauge kinetic functions and the FI-terms. Minimize

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Year of Publication:

2013-09-30

Source:

http://arxiv.org/pdf/0705.2366v1.pdf

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Non-perturbative SQCD superpotentials from string instantons

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The Affleck–Dine–Seiberg instanton generated superpotential for SQCD with Nf = Nc − 1 flavours is explicitly derived from a local model of engineered intersecting D6-branes with a single E2-instanton. This computation extends also to symplectic gauge groups with Nf = Nc flavours.

The Affleck–Dine–Seiberg instanton generated superpotential for SQCD with Nf = Nc − 1 flavours is explicitly derived from a local model of engineered intersecting D6-branes with a single E2-instanton. This computation extends also to symplectic gauge groups with Nf = Nc flavours. Minimize

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Year of Publication:

2013-09-30

Source:

http://arxiv.org/pdf/hep-th/0612132v1.pdf

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Non-perturbative SQCD superpotentials from string instantons

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The Affleck–Dine–Seiberg instanton generated superpotential for SQCD with Nf = Nc − 1 flavours is explicitly derived from a local model of engineered intersecting D6-branes with a single E2-instanton. This computation extends also to symplectic gauge groups with Nf = Nc flavours.

The Affleck–Dine–Seiberg instanton generated superpotential for SQCD with Nf = Nc − 1 flavours is explicitly derived from a local model of engineered intersecting D6-branes with a single E2-instanton. This computation extends also to symplectic gauge groups with Nf = Nc flavours. Minimize

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The Pennsylvania State University CiteSeerX Archives

Year of Publication:

2013-09-30

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http://arxiv.org/pdf/hep-th/0612132v2.pdf

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Non-perturbative SQCD superpotentials from string instantons

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The Affleck–Dine–Seiberg instanton generated superpotential for SQCD with Nf = Nc − 1 flavours is explicitly derived from a local model of engineered intersecting D6-branes with a single E2-instanton. This computation extends also to symplectic gauge groups with Nf = Nc flavours.

The Affleck–Dine–Seiberg instanton generated superpotential for SQCD with Nf = Nc − 1 flavours is explicitly derived from a local model of engineered intersecting D6-branes with a single E2-instanton. This computation extends also to symplectic gauge groups with Nf = Nc flavours. Minimize

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The Pennsylvania State University CiteSeerX Archives

Year of Publication:

2013-09-30

Source:

http://arxiv.org/pdf/hep-th/0612132v3.pdf

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