Two equivalent definitions of fibration structure on toric CY $3$-foldequivalent definitions of orientationEquivalent definitions of Kähler metricAre these two definitions of $EG$ equivalent?Equivalent definitions of “evenly covered”Existence of real structure on CY m-foldModuli Space of elliptic fibrationEquivalence of two definitions of Spin structureEquivalent definitions of “meromorphic section”?Recovering data about the toric fan from minimal informationQuestion about differential forms and delta functions

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Two equivalent definitions of fibration structure on toric CY $3$-fold


equivalent definitions of orientationEquivalent definitions of Kähler metricAre these two definitions of $EG$ equivalent?Equivalent definitions of “evenly covered”Existence of real structure on CY m-foldModuli Space of elliptic fibrationEquivalence of two definitions of Spin structureEquivalent definitions of “meromorphic section”?Recovering data about the toric fan from minimal informationQuestion about differential forms and delta functions













1












$begingroup$


I've been trying to reconcile two seemingly different definitions of what a toric space is, specifically a toric Calabi-Yau 3-fold. The first definition is from the paper Branes and Toric Geometry, by Leung and Vafa (arXiv:hep-th/9711013) who say (on page 12, section 2.1):




We are interested in manifolds admitting a $T^n$ action, with an $n$-dimensional base.




This seems to suggest that a toric Calabi-Yau $3$-fold (generalizing the construction in the paper) is a $T^3$ fibration over a real $3$-dimensional base.



However, in the thesis Crystal Melting and Wall Crossing Phenomena, by Yamazaki (arXiv:1002.1709 [hep-th]), the author explicitly says (on page 16, in section 3.2):




A toric Calabi-Yau threefold $X_Delta$ is a $T^2 times mathbbR$ fibration over $mathbbR^3$, where the fibers are special Lagrangian submanifolds.




Now I understand that the phrase "special Lagrangian submanifold" implies the existence in $X_Delta$ of a special Lagrangian submanifold. But I would like to know the sense in which these two seemingly different definitions are equivalent. Any references to a further discussion about toric spaces would is very welcome! (I am a physicist learning about the underlying mathematical structures. I would not like to shy away from the formal definitions, so math references are particularly welcome.)










share|cite|improve this question











$endgroup$











  • $begingroup$
    The answer is in section 4.3 of Vincent Bouchard's lecture notes at arxiv.org/abs/hep-th/0702063. I would like to see the Lagrangian submanifold structure more explicitly but I guess I just need to work it out.
    $endgroup$
    – leastaction
    Mar 30 at 15:22















1












$begingroup$


I've been trying to reconcile two seemingly different definitions of what a toric space is, specifically a toric Calabi-Yau 3-fold. The first definition is from the paper Branes and Toric Geometry, by Leung and Vafa (arXiv:hep-th/9711013) who say (on page 12, section 2.1):




We are interested in manifolds admitting a $T^n$ action, with an $n$-dimensional base.




This seems to suggest that a toric Calabi-Yau $3$-fold (generalizing the construction in the paper) is a $T^3$ fibration over a real $3$-dimensional base.



However, in the thesis Crystal Melting and Wall Crossing Phenomena, by Yamazaki (arXiv:1002.1709 [hep-th]), the author explicitly says (on page 16, in section 3.2):




A toric Calabi-Yau threefold $X_Delta$ is a $T^2 times mathbbR$ fibration over $mathbbR^3$, where the fibers are special Lagrangian submanifolds.




Now I understand that the phrase "special Lagrangian submanifold" implies the existence in $X_Delta$ of a special Lagrangian submanifold. But I would like to know the sense in which these two seemingly different definitions are equivalent. Any references to a further discussion about toric spaces would is very welcome! (I am a physicist learning about the underlying mathematical structures. I would not like to shy away from the formal definitions, so math references are particularly welcome.)










share|cite|improve this question











$endgroup$











  • $begingroup$
    The answer is in section 4.3 of Vincent Bouchard's lecture notes at arxiv.org/abs/hep-th/0702063. I would like to see the Lagrangian submanifold structure more explicitly but I guess I just need to work it out.
    $endgroup$
    – leastaction
    Mar 30 at 15:22













1












1








1


1



$begingroup$


I've been trying to reconcile two seemingly different definitions of what a toric space is, specifically a toric Calabi-Yau 3-fold. The first definition is from the paper Branes and Toric Geometry, by Leung and Vafa (arXiv:hep-th/9711013) who say (on page 12, section 2.1):




We are interested in manifolds admitting a $T^n$ action, with an $n$-dimensional base.




This seems to suggest that a toric Calabi-Yau $3$-fold (generalizing the construction in the paper) is a $T^3$ fibration over a real $3$-dimensional base.



However, in the thesis Crystal Melting and Wall Crossing Phenomena, by Yamazaki (arXiv:1002.1709 [hep-th]), the author explicitly says (on page 16, in section 3.2):




A toric Calabi-Yau threefold $X_Delta$ is a $T^2 times mathbbR$ fibration over $mathbbR^3$, where the fibers are special Lagrangian submanifolds.




Now I understand that the phrase "special Lagrangian submanifold" implies the existence in $X_Delta$ of a special Lagrangian submanifold. But I would like to know the sense in which these two seemingly different definitions are equivalent. Any references to a further discussion about toric spaces would is very welcome! (I am a physicist learning about the underlying mathematical structures. I would not like to shy away from the formal definitions, so math references are particularly welcome.)










share|cite|improve this question











$endgroup$




I've been trying to reconcile two seemingly different definitions of what a toric space is, specifically a toric Calabi-Yau 3-fold. The first definition is from the paper Branes and Toric Geometry, by Leung and Vafa (arXiv:hep-th/9711013) who say (on page 12, section 2.1):




We are interested in manifolds admitting a $T^n$ action, with an $n$-dimensional base.




This seems to suggest that a toric Calabi-Yau $3$-fold (generalizing the construction in the paper) is a $T^3$ fibration over a real $3$-dimensional base.



However, in the thesis Crystal Melting and Wall Crossing Phenomena, by Yamazaki (arXiv:1002.1709 [hep-th]), the author explicitly says (on page 16, in section 3.2):




A toric Calabi-Yau threefold $X_Delta$ is a $T^2 times mathbbR$ fibration over $mathbbR^3$, where the fibers are special Lagrangian submanifolds.




Now I understand that the phrase "special Lagrangian submanifold" implies the existence in $X_Delta$ of a special Lagrangian submanifold. But I would like to know the sense in which these two seemingly different definitions are equivalent. Any references to a further discussion about toric spaces would is very welcome! (I am a physicist learning about the underlying mathematical structures. I would not like to shy away from the formal definitions, so math references are particularly welcome.)







algebraic-topology mathematical-physics complex-geometry toric-geometry string-theory






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Mar 22 at 14:31









Andrews

1,2812423




1,2812423










asked Mar 9 at 21:02









leastactionleastaction

283111




283111











  • $begingroup$
    The answer is in section 4.3 of Vincent Bouchard's lecture notes at arxiv.org/abs/hep-th/0702063. I would like to see the Lagrangian submanifold structure more explicitly but I guess I just need to work it out.
    $endgroup$
    – leastaction
    Mar 30 at 15:22
















  • $begingroup$
    The answer is in section 4.3 of Vincent Bouchard's lecture notes at arxiv.org/abs/hep-th/0702063. I would like to see the Lagrangian submanifold structure more explicitly but I guess I just need to work it out.
    $endgroup$
    – leastaction
    Mar 30 at 15:22















$begingroup$
The answer is in section 4.3 of Vincent Bouchard's lecture notes at arxiv.org/abs/hep-th/0702063. I would like to see the Lagrangian submanifold structure more explicitly but I guess I just need to work it out.
$endgroup$
– leastaction
Mar 30 at 15:22




$begingroup$
The answer is in section 4.3 of Vincent Bouchard's lecture notes at arxiv.org/abs/hep-th/0702063. I would like to see the Lagrangian submanifold structure more explicitly but I guess I just need to work it out.
$endgroup$
– leastaction
Mar 30 at 15:22










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