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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3639 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6115 | 0.781 | 0.783 | [M:[1.0, 0.8992, 0.7122, 1.2878, 0.7626], q:[0.7626, 0.2374], qb:[0.5252, 0.5756], phi:[0.4748]] | [M:[[0], [-8], [-3], [3], [1]], q:[[1], [-1]], qb:[[2], [6]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}^{4}$ | ${}$ | -3 | 2*t^2.288 + t^2.439 + t^2.698 + 2*t^2.849 + t^3. + 2*t^3.863 + t^4.014 + 4*t^4.576 + 3*t^4.727 + 2*t^4.878 + t^4.986 + 4*t^5.137 + 4*t^5.288 + t^5.395 + t^5.439 + 2*t^5.547 + 4*t^5.698 - 3*t^6. + 2*t^6.151 + 3*t^6.302 - t^6.41 + t^6.453 + 2*t^6.712 + 6*t^6.863 + 4*t^7.014 + 4*t^7.166 + t^7.273 + 2*t^7.317 + 5*t^7.424 + 6*t^7.576 + t^7.683 + 6*t^7.727 + 2*t^7.834 + 2*t^7.878 + 7*t^7.986 + t^8.093 + 3*t^8.137 + 2*t^8.244 - 7*t^8.288 + 4*t^8.395 - 2*t^8.439 + 5*t^8.547 + 3*t^8.59 - 4*t^8.698 + 5*t^8.741 - 9*t^8.849 + 2*t^8.892 - t^4.424/y - t^6.712/y - t^7.122/y - t^7.273/y + (2*t^7.576)/y + (3*t^7.727)/y + (2*t^7.986)/y + (6*t^8.137)/y + (4*t^8.288)/y + t^8.439/y + (2*t^8.547)/y + (2*t^8.698)/y + (2*t^8.849)/y - t^4.424*y - t^6.712*y - t^7.122*y - t^7.273*y + 2*t^7.576*y + 3*t^7.727*y + 2*t^7.986*y + 6*t^8.137*y + 4*t^8.288*y + t^8.439*y + 2*t^8.547*y + 2*t^8.698*y + 2*t^8.849*y | 2*g1*t^2.288 + g1^5*t^2.439 + t^2.698/g1^8 + (2*t^2.849)/g1^4 + t^3. + 2*g1^3*t^3.863 + g1^7*t^4.014 + 4*g1^2*t^4.576 + 3*g1^6*t^4.727 + 2*g1^10*t^4.878 + t^4.986/g1^7 + (4*t^5.137)/g1^3 + 4*g1*t^5.288 + t^5.395/g1^16 + g1^5*t^5.439 + (2*t^5.547)/g1^12 + (4*t^5.698)/g1^8 - 3*t^6. + 2*g1^4*t^6.151 + 3*g1^8*t^6.302 - t^6.41/g1^9 + g1^12*t^6.453 + (2*t^6.712)/g1 + 6*g1^3*t^6.863 + 4*g1^7*t^7.014 + 4*g1^11*t^7.166 + t^7.273/g1^6 + 2*g1^15*t^7.317 + (5*t^7.424)/g1^2 + 6*g1^2*t^7.576 + t^7.683/g1^15 + 6*g1^6*t^7.727 + (2*t^7.834)/g1^11 + 2*g1^10*t^7.878 + (7*t^7.986)/g1^7 + t^8.093/g1^24 + (3*t^8.137)/g1^3 + (2*t^8.244)/g1^20 - 7*g1*t^8.288 + (4*t^8.395)/g1^16 - 2*g1^5*t^8.439 + (5*t^8.547)/g1^12 + 3*g1^9*t^8.59 - (4*t^8.698)/g1^8 + 5*g1^13*t^8.741 - (9*t^8.849)/g1^4 + 2*g1^17*t^8.892 - t^4.424/(g1^2*y) - t^6.712/(g1*y) - t^7.122/(g1^10*y) - t^7.273/(g1^6*y) + (2*g1^2*t^7.576)/y + (3*g1^6*t^7.727)/y + (2*t^7.986)/(g1^7*y) + (6*t^8.137)/(g1^3*y) + (4*g1*t^8.288)/y + (g1^5*t^8.439)/y + (2*t^8.547)/(g1^12*y) + (2*t^8.698)/(g1^8*y) + (2*t^8.849)/(g1^4*y) - (t^4.424*y)/g1^2 - (t^6.712*y)/g1 - (t^7.122*y)/g1^10 - (t^7.273*y)/g1^6 + 2*g1^2*t^7.576*y + 3*g1^6*t^7.727*y + (2*t^7.986*y)/g1^7 + (6*t^8.137*y)/g1^3 + 4*g1*t^8.288*y + g1^5*t^8.439*y + (2*t^8.547*y)/g1^12 + (2*t^8.698*y)/g1^8 + (2*t^8.849*y)/g1^4 |
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 |
---|---|---|---|---|---|---|---|---|---|
3221 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ | 0.5931 | 0.7477 | 0.7932 | [M:[1.0, 0.8948, 0.7105, 1.2895], q:[0.7632, 0.2368], qb:[0.5263, 0.5789], phi:[0.4737]] | t^2.289 + t^2.447 + t^2.684 + 2*t^2.842 + t^3. + t^3.711 + 2*t^3.868 + t^4.026 + 2*t^4.579 + 2*t^4.737 + 2*t^4.895 + 2*t^5.132 + 3*t^5.289 + t^5.369 + t^5.447 + 2*t^5.527 + 4*t^5.684 - 2*t^6. - t^4.421/y - t^4.421*y | detail |