Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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1300 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}^{2}$ + ${ }M_{2}M_{6}$ | 0.7136 | 0.8827 | 0.8085 | [M:[0.9544, 1.0912, 0.8177, 0.9088, 1.0, 0.9088], q:[0.4316, 0.614], qb:[0.4772, 0.5684], phi:[0.4772]] | [M:[[-2], [4], [-8], [-4], [0], [-4]], q:[[-3], [5]], qb:[[-1], [3]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }M_{4}$, ${ }M_{6}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{5}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{1}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.453 + 2*t^2.727 + 2*t^2.863 + t^3. + t^3.137 + t^4.021 + t^4.158 + t^4.295 + t^4.432 + 2*t^4.568 + t^4.705 + t^4.842 + t^4.906 + t^4.979 + t^5.115 + 2*t^5.18 + 2*t^5.316 + 3*t^5.453 + 3*t^5.59 + 4*t^5.727 + 2*t^5.863 - t^6. - t^6.137 - t^6.273 - 2*t^6.41 + t^6.474 - t^6.547 + t^6.611 + 3*t^6.748 + 4*t^6.885 + 5*t^7.021 + 4*t^7.158 + 4*t^7.295 + t^7.359 + 4*t^7.432 + 3*t^7.568 + 2*t^7.633 + t^7.705 + 2*t^7.769 + t^7.842 + 3*t^7.906 + t^7.979 + 4*t^8.043 - t^8.115 + 7*t^8.18 - t^8.252 + 4*t^8.316 + 4*t^8.453 + 6*t^8.59 - 3*t^8.727 - 4*t^8.863 + t^8.927 - t^4.432/y - t^6.885/y - t^7.158/y - (2*t^7.295)/y + (2*t^7.568)/y + t^7.705/y + t^7.979/y + (2*t^8.18)/y + (2*t^8.316)/y + (2*t^8.453)/y + (5*t^8.59)/y + (3*t^8.727)/y + (4*t^8.863)/y - t^4.432*y - t^6.885*y - t^7.158*y - 2*t^7.295*y + 2*t^7.568*y + t^7.705*y + t^7.979*y + 2*t^8.18*y + 2*t^8.316*y + 2*t^8.453*y + 5*t^8.59*y + 3*t^8.727*y + 4*t^8.863*y | t^2.453/g1^8 + (2*t^2.727)/g1^4 + (2*t^2.863)/g1^2 + t^3. + g1^2*t^3.137 + t^4.021/g1^7 + t^4.158/g1^5 + t^4.295/g1^3 + t^4.432/g1 + 2*g1*t^4.568 + g1^3*t^4.705 + g1^5*t^4.842 + t^4.906/g1^16 + g1^7*t^4.979 + g1^9*t^5.115 + (2*t^5.18)/g1^12 + (2*t^5.316)/g1^10 + (3*t^5.453)/g1^8 + (3*t^5.59)/g1^6 + (4*t^5.727)/g1^4 + (2*t^5.863)/g1^2 - t^6. - g1^2*t^6.137 - g1^4*t^6.273 - 2*g1^6*t^6.41 + t^6.474/g1^15 - g1^8*t^6.547 + t^6.611/g1^13 + (3*t^6.748)/g1^11 + (4*t^6.885)/g1^9 + (5*t^7.021)/g1^7 + (4*t^7.158)/g1^5 + (4*t^7.295)/g1^3 + t^7.359/g1^24 + (4*t^7.432)/g1 + 3*g1*t^7.568 + (2*t^7.633)/g1^20 + g1^3*t^7.705 + (2*t^7.769)/g1^18 + g1^5*t^7.842 + (3*t^7.906)/g1^16 + g1^7*t^7.979 + (4*t^8.043)/g1^14 - g1^9*t^8.115 + (7*t^8.18)/g1^12 - g1^11*t^8.252 + (4*t^8.316)/g1^10 + (4*t^8.453)/g1^8 + (6*t^8.59)/g1^6 - (3*t^8.727)/g1^4 - (4*t^8.863)/g1^2 + t^8.927/g1^23 - t^4.432/(g1*y) - t^6.885/(g1^9*y) - t^7.158/(g1^5*y) - (2*t^7.295)/(g1^3*y) + (2*g1*t^7.568)/y + (g1^3*t^7.705)/y + (g1^7*t^7.979)/y + (2*t^8.18)/(g1^12*y) + (2*t^8.316)/(g1^10*y) + (2*t^8.453)/(g1^8*y) + (5*t^8.59)/(g1^6*y) + (3*t^8.727)/(g1^4*y) + (4*t^8.863)/(g1^2*y) - (t^4.432*y)/g1 - (t^6.885*y)/g1^9 - (t^7.158*y)/g1^5 - (2*t^7.295*y)/g1^3 + 2*g1*t^7.568*y + g1^3*t^7.705*y + g1^7*t^7.979*y + (2*t^8.18*y)/g1^12 + (2*t^8.316*y)/g1^10 + (2*t^8.453*y)/g1^8 + (5*t^8.59*y)/g1^6 + (3*t^8.727*y)/g1^4 + (4*t^8.863*y)/g1^2 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
823 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}^{2}$ | 0.706 | 0.8681 | 0.8132 | [M:[0.9624, 1.0751, 0.8498, 0.9249, 1.0], q:[0.4437, 0.5939], qb:[0.4812, 0.5563], phi:[0.4812]] | t^2.549 + t^2.775 + 2*t^2.887 + t^3. + t^3.113 + t^3.225 + t^4.106 + t^4.218 + t^4.331 + t^4.444 + 2*t^4.556 + t^4.669 + t^4.782 + t^4.894 + t^5.007 + t^5.099 + t^5.324 + 2*t^5.437 + t^5.549 + t^5.662 + 4*t^5.775 + t^5.887 - t^4.444/y - t^4.444*y | detail |