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Mirror Fermat Calabi-Yau Threefolds and Landau-Ginzburg Black Hole Attractors
We study black hole attractor equations for one-(complex structure)modulus Calabi-Yau spaces which are the mirror dual of Fermat Calabi-Yau threefolds (CY_{3}s). When exploring non-degenerate solutions near the Landau-Ginzburg point of the moduli space of such 4-dimensional compactifications, we alw...
Autores principales: | , , , |
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Lenguaje: | eng |
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2006
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Acceso en línea: | https://dx.doi.org/10.1393/ncr/i2007-10013-y http://cds.cern.ch/record/978076 |
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author | Bellucci, Stefano Ferrara, Sergio Marrani, Alessio Yeranyan, Armen |
author_facet | Bellucci, Stefano Ferrara, Sergio Marrani, Alessio Yeranyan, Armen |
author_sort | Bellucci, Stefano |
collection | CERN |
description | We study black hole attractor equations for one-(complex structure)modulus Calabi-Yau spaces which are the mirror dual of Fermat Calabi-Yau threefolds (CY_{3}s). When exploring non-degenerate solutions near the Landau-Ginzburg point of the moduli space of such 4-dimensional compactifications, we always find two species of extremal black hole attractors, depending on the choice of the Sp(4,Z) symplectic charge vector, one 1/2-BPS (which is always stable, according to general results of special Kahler geometry) and one non-BPS. The latter turns out to be stable (local minimum of the ``effective black hole potential'' V_{BH}) for non-vanishing central charge, whereas it is unstable (saddle point of V_{BH}) for the case of vanishing central charge. This is to be compared to the large volume limit of one-modulus CY_{3}-compactifications (of Type II A superstrings), in which the homogeneous symmetric special Kahler geometry based on cubic prepotential admits (beside the 1/2-BPS ones) only non-BPS extremal black hole attractors with non-vanishing central charge, which are always stable. |
id | cern-978076 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2006 |
record_format | invenio |
spelling | cern-9780762021-02-02T03:00:45Zdoi:10.1393/ncr/i2007-10013-yhttp://cds.cern.ch/record/978076engBellucci, StefanoFerrara, SergioMarrani, AlessioYeranyan, ArmenMirror Fermat Calabi-Yau Threefolds and Landau-Ginzburg Black Hole AttractorsParticle Physics - TheoryWe study black hole attractor equations for one-(complex structure)modulus Calabi-Yau spaces which are the mirror dual of Fermat Calabi-Yau threefolds (CY_{3}s). When exploring non-degenerate solutions near the Landau-Ginzburg point of the moduli space of such 4-dimensional compactifications, we always find two species of extremal black hole attractors, depending on the choice of the Sp(4,Z) symplectic charge vector, one 1/2-BPS (which is always stable, according to general results of special Kahler geometry) and one non-BPS. The latter turns out to be stable (local minimum of the ``effective black hole potential'' V_{BH}) for non-vanishing central charge, whereas it is unstable (saddle point of V_{BH}) for the case of vanishing central charge. This is to be compared to the large volume limit of one-modulus CY_{3}-compactifications (of Type II A superstrings), in which the homogeneous symmetric special Kahler geometry based on cubic prepotential admits (beside the 1/2-BPS ones) only non-BPS extremal black hole attractors with non-vanishing central charge, which are always stable.We study black hole attractor equations for one-(complex structure)modulus Calabi-Yau spaces which are the mirror dual of Fermat Calabi-Yau threefolds (CY_{3}s). When exploring non-degenerate solutions near the Landau-Ginzburg point of the moduli space of such 4-dimensional compactifications, we always find two species of extremal black hole attractors, depending on the choice of the Sp(4,Z) symplectic charge vector, one 1/2-BPS (which is always stable, according to general results of special Kahler geometry) and one non-BPS. The latter turns out to be stable (local minimum of the ``effective black hole potential'' V_{BH}) for non-vanishing central charge, whereas it is unstable (saddle point of V_{BH}) for the case of vanishing central charge. This is to be compared to the large volume limit of one-modulus CY_{3}-compactifications (of Type II A superstrings), in which the homogeneous symmetric special Kahler geometry based on cubic prepotential admits (beside the 1/2-BPS ones) only non-BPS extremal black hole attractors with non-vanishing central charge, which are always stable.We study black hole attractor equations for one-(complex structure)modulus Calabi-Yau spaces which are the mirror dual of Fermat Calabi-Yau threefolds (CY_{3}s). When exploring non-degenerate solutions near the Landau-Ginzburg point of the moduli space of such 4-dimensional compactifications, we always find two species of extremal black hole attractors, depending on the choice of the Sp(4,Z) symplectic charge vector, one 1/2-BPS (which is always stable, according to general results of special Kahler geometry) and one non-BPS. The latter turns out to be stable (local minimum of the ``effective black hole potential'' V_{BH}) for non-vanishing central charge, whereas it is unstable (saddle point of V_{BH}) for the case of vanishing central charge. This is to be compared to the large volume limit of one-modulus CY_{3}-compactifications (of Type II A superstrings), in which the homogeneous symmetric special Kahler geometry based on cubic prepotential admits (beside the 1/2-BPS ones) only non-BPS extremal black hole attractors with non-vanishing central charge, which are always stable.We discuss the “attractor mechanism” for extremal black-holes (BHs) in the context of Maxwell-Einstein supergravity theories. The BH squared mass at the horizon (related to the Bekenstein-Hawking entropy area formula) is determined by the “fixed points” of the so-called “BH potential”. In the considered framework, the scalar fields describe trajectories ending into such fixed points, which only depend on the electric and magnetic BH charges. Thus, the BH appears as a soliton, interpolating between maximally supersymmetric limiting solutions at spatial infinity and at the horizon. The BH entropy depend only on the BH charges, and it is independent of the initial data, i.e. on the values of the scalar fields at spatial infinity. In the considered theories, extremal BHs seem to behave as dynamical systems with fixed points (“attractors”) describing the thermodynamical equilibrium and stability features. An introductory review of the “special Kahler” geometry for scalar manifolds encompassing the BH background is given. A detailed study of the BH attractor equations for one-(complex structure)modulus Calabi-Yau spaces which are the mirror dual of Fermat Calabi-Yau threefolds (CY$_{3}$’s) is carried out as well. When exploring non-degenerate solutions near the Landau-Ginzburg point of the moduli space of such 4-dimensional compactifications, we always find two species of extremal black-hole attractors, depending on the choice of the Sp(4, ℤ) symplectic charge vector, one $\frac{1}{2}$-BPS (which is always stable, according to general results of special Kahler geometry) and one non-BPS. The latter turns out to be stable (local minimum of the “effective black-hole potential” V$_{bh}$) for non-vanishing central charge, whereas it is unstable (saddle point of V$_{BH}$) for the case of vanishing central charge. This is to be compared to the large volume limit of one-modulus CY$_{3}$-compactifications (of type-IIA superstrings), in which the homogeneous symmetric special Kahler geometry based on cubic prepotential admits (beside the $\frac{1}{2}$-BPS ones) only non-BPS extremal black-hole attractors with non-vanishing central charge, which are always stable.hep-th/0608091CERN-PH-TH-2006-154CERN-PH-TH-2006-154oai:cds.cern.ch:9780762006-08-14 |
spellingShingle | Particle Physics - Theory Bellucci, Stefano Ferrara, Sergio Marrani, Alessio Yeranyan, Armen Mirror Fermat Calabi-Yau Threefolds and Landau-Ginzburg Black Hole Attractors |
title | Mirror Fermat Calabi-Yau Threefolds and Landau-Ginzburg Black Hole Attractors |
title_full | Mirror Fermat Calabi-Yau Threefolds and Landau-Ginzburg Black Hole Attractors |
title_fullStr | Mirror Fermat Calabi-Yau Threefolds and Landau-Ginzburg Black Hole Attractors |
title_full_unstemmed | Mirror Fermat Calabi-Yau Threefolds and Landau-Ginzburg Black Hole Attractors |
title_short | Mirror Fermat Calabi-Yau Threefolds and Landau-Ginzburg Black Hole Attractors |
title_sort | mirror fermat calabi-yau threefolds and landau-ginzburg black hole attractors |
topic | Particle Physics - Theory |
url | https://dx.doi.org/10.1393/ncr/i2007-10013-y http://cds.cern.ch/record/978076 |
work_keys_str_mv | AT belluccistefano mirrorfermatcalabiyauthreefoldsandlandauginzburgblackholeattractors AT ferrarasergio mirrorfermatcalabiyauthreefoldsandlandauginzburgblackholeattractors AT marranialessio mirrorfermatcalabiyauthreefoldsandlandauginzburgblackholeattractors AT yeranyanarmen mirrorfermatcalabiyauthreefoldsandlandauginzburgblackholeattractors |