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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79612 | Sp2s2nf1 | ${}M_{1}S_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }M_{2}S_{2}^{2}$ + ${ }M_{3}S_{2}^{2}$ + ${ }q_{1}^{2}S_{1}$ | 2.369 | 2.5155 | 0.9418 | [X:[], M:[0.9251, 0.8062, 0.8062], q:[0.7313, 0.4625], qb:[], phi:[], S:[0.5375, 0.5969], Sb:[], A:[], Ab:[]] | [X:[], M:[[8], [-6], [-6]], q:[[2], [4]], qb:[], phi:[], S:[[-4], [3]], Sb:[], A:[], Ab:[]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }S_{1}S_{2}$, ${ }q_{2}^{2}S_{1}$, ${ }q_{2}^{2}S_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{3}$, ${ }q_{1}q_{2}S_{1}$, ${ }q_{1}q_{2}S_{2}$, ${ }M_{1}^{2}$, ${ }M_{3}S_{1}S_{2}$ | ${}$ | -2 | 2*t^2.419 + t^2.775 + t^3.403 + t^4.388 + t^4.566 + 3*t^4.837 + 2*t^5.194 + t^5.372 + t^5.55 + t^5.822 - 2*t^6. + 2*t^6.178 + t^6.45 + t^6.628 + 4*t^6.806 + 3*t^6.984 + 2*t^7.163 + 4*t^7.256 + t^7.341 + 3*t^7.612 + 3*t^7.791 + 4*t^7.969 + 2*t^8.147 + t^8.24 + t^8.326 - 4*t^8.419 + 2*t^8.597 + 2*t^8.868 + 3*t^8.953 - t^4.612/y - t^4.791/y - (2*t^7.031)/y - t^7.209/y - t^7.566/y - (2*t^8.016)/y - t^8.372/y + (2*t^8.822)/y - t^4.612*y - t^4.791*y - 2*t^7.031*y - t^7.209*y - t^7.566*y - 2*t^8.016*y - t^8.372*y + 2*t^8.822*y | (2*t^2.419)/g1^6 + g1^8*t^2.775 + t^3.403/g1 + g1^4*t^4.388 + g1^11*t^4.566 + (3*t^4.837)/g1^12 + 2*g1^2*t^5.194 + g1^9*t^5.372 + g1^16*t^5.55 + t^5.822/g1^7 - 2*t^6. + 2*g1^7*t^6.178 + t^6.45/g1^16 + t^6.628/g1^9 + (4*t^6.806)/g1^2 + 3*g1^5*t^6.984 + 2*g1^12*t^7.163 + (4*t^7.256)/g1^18 + g1^19*t^7.341 + (3*t^7.612)/g1^4 + 3*g1^3*t^7.791 + 4*g1^10*t^7.969 + 2*g1^17*t^8.147 + t^8.24/g1^13 + g1^24*t^8.326 - (4*t^8.419)/g1^6 + 2*g1*t^8.597 + (2*t^8.868)/g1^22 + 3*g1^15*t^8.953 - t^4.612/(g1^4*y) - (g1^3*t^4.791)/y - (2*t^7.031)/(g1^10*y) - t^7.209/(g1^3*y) - (g1^11*t^7.566)/y - (2*t^8.016)/(g1^5*y) - (g1^9*t^8.372)/y + (2*t^8.822)/(g1^7*y) - (t^4.612*y)/g1^4 - g1^3*t^4.791*y - (2*t^7.031*y)/g1^10 - (t^7.209*y)/g1^3 - g1^11*t^7.566*y - (2*t^8.016*y)/g1^5 - g1^9*t^8.372*y + (2*t^8.822*y)/g1^7 |
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 |
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79543 | Sp2s2nf1 | ${}M_{1}S_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }M_{2}S_{2}^{2}$ + ${ }M_{3}S_{2}^{2}$ | 2.4204 | 2.5694 | 0.942 | [X:[], M:[0.8921, 0.8309, 0.8309], q:[0.5846, 0.5846], qb:[], phi:[], S:[0.5539, 0.5846], Sb:[], A:[], Ab:[]] | 2*t^2.493 + t^2.676 + t^3.415 + 3*t^4.985 + 5*t^5.169 + 3*t^5.261 + t^5.353 + t^5.908 - 5*t^6. - t^4.662/y - t^4.754/y - t^4.662*y - t^4.754*y | detail |