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Bogomolny-Prasad-Sommerfeld state counting in local obstructed curves from quiver theory and Seiberg duality
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10.1063/1.3364787
/content/aip/journal/jmp/51/5/10.1063/1.3364787
http://aip.metastore.ingenta.com/content/aip/journal/jmp/51/5/10.1063/1.3364787

Figures

Image of FIG. 1.
FIG. 1.

This is the chamber structure of the original conifold quiver with only one framing arrow.

Image of FIG. 2.
FIG. 2.

This is the ERC for affine quiver with superpotential degree and one framing arrow, which is not reversed. It is denoted by infinite ERC.

Image of FIG. 3.
FIG. 3.

This is the ERC for affine quiver with superpotential degree and three framing arrows, denoted by finite ERC.

Image of FIG. 4.
FIG. 4.

An example of the filtered pyramid partitions of finite ERC .

Image of FIG. 5.
FIG. 5.

This figure shows the three fixed point in Example 2.

Image of FIG. 6.
FIG. 6.

The single fixed point for dimension vector .

Image of FIG. 7.
FIG. 7.

Four fixed points for .

Tables

Generic image for table
Table I.

All bifundamental fields after the mutation.

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/content/aip/journal/jmp/51/5/10.1063/1.3364787
2010-05-20
2014-04-17
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Bogomolny-Prasad-Sommerfeld state counting in local obstructed curves from quiver theory and Seiberg duality
http://aip.metastore.ingenta.com/content/aip/journal/jmp/51/5/10.1063/1.3364787
10.1063/1.3364787
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