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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61260 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ | 1.3956 | 1.6375 | 0.8523 | [X:[], M:[0.7648, 1.2, 1.1648], q:[0.4213, 0.3894], qb:[0.4139, 0.3754], phi:[0.4]] | [X:[], M:[[1, 2], [0, 0], [1, 2]], q:[[-2, -2], [1, 1]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{3}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | ${2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | 2*t^2.29 + t^2.39 + t^2.41 + 2*t^3.49 + t^3.59 + 2*t^3.6 + t^3.61 + 3*t^4.59 + 2*t^4.68 + 2*t^4.69 + 2*t^4.7 + t^4.78 + t^4.79 + 2*t^4.8 + 2*t^4.81 + t^4.82 + t^4.9 + t^4.91 + 4*t^5.79 + 3*t^5.88 + 5*t^5.89 + 3*t^5.9 + t^5.98 + 2*t^5.99 - t^6. + 3*t^6.01 + t^6.02 - t^6.12 + 4*t^6.88 + 4*t^6.98 + 7*t^6.99 + 3*t^7. + 2*t^7.07 + 5*t^7.08 + 8*t^7.09 + 7*t^7.1 + 2*t^7.11 + t^7.17 + 2*t^7.18 + 4*t^7.19 + 5*t^7.2 + 4*t^7.21 + 3*t^7.22 + t^7.23 + t^7.29 + t^7.3 - t^7.31 + t^7.33 + t^7.39 + 6*t^8.08 + 5*t^8.18 + 11*t^8.19 + 5*t^8.2 + 3*t^8.27 + 7*t^8.28 + t^8.29 + 9*t^8.3 + 3*t^8.31 + t^8.37 + 3*t^8.38 + 3*t^8.4 - t^8.41 + 4*t^8.42 + t^8.43 + t^8.5 - 2*t^8.51 - t^8.52 - t^8.53 - t^8.6 - t^4.2/y - t^5.4/y - (2*t^6.49)/y - t^6.59/y - t^6.61/y + t^7.59/y + (2*t^7.68)/y - (3*t^7.69)/y + (2*t^7.7)/y - t^7.79/y - t^7.81/y + t^7.91/y + t^8.79/y + (2*t^8.88)/y + (2*t^8.89)/y + (2*t^8.9)/y + t^8.99/y - t^4.2*y - t^5.4*y - 2*t^6.49*y - t^6.59*y - t^6.61*y + t^7.59*y + 2*t^7.68*y - 3*t^7.69*y + 2*t^7.7*y - t^7.79*y - t^7.81*y + t^7.91*y + t^8.79*y + 2*t^8.88*y + 2*t^8.89*y + 2*t^8.9*y + t^8.99*y | 2*g1*g2^2*t^2.29 + t^2.39/(g1^2*g2) + g1^2*g2*t^2.41 + 2*g1*g2^2*t^3.49 + t^3.59/(g1^2*g2) + 2*t^3.6 + g1^2*g2*t^3.61 + 3*g1^2*g2^4*t^4.59 + (2*g2*t^4.68)/g1 + 2*g1*g2^2*t^4.69 + 2*g1^3*g2^3*t^4.7 + t^4.78/(g1^4*g2^2) + t^4.79/(g1^2*g2) + 2*t^4.8 + 2*g1^2*g2*t^4.81 + g1^4*g2^2*t^4.82 + t^4.9/(g1^3*g2^3) + t^4.91/(g1*g2^2) + 4*g1^2*g2^4*t^5.79 + (3*g2*t^5.88)/g1 + 5*g1*g2^2*t^5.89 + 3*g1^3*g2^3*t^5.9 + t^5.98/(g1^4*g2^2) + (2*t^5.99)/(g1^2*g2) - t^6. + 3*g1^2*g2*t^6.01 + g1^4*g2^2*t^6.02 - (g1*t^6.12)/g2 + 4*g1^3*g2^6*t^6.88 + 4*g2^3*t^6.98 + 7*g1^2*g2^4*t^6.99 + 3*g1^4*g2^5*t^7. + (2*t^7.07)/g1^3 + (5*g2*t^7.08)/g1 + 8*g1*g2^2*t^7.09 + 7*g1^3*g2^3*t^7.1 + 2*g1^5*g2^4*t^7.11 + t^7.17/(g1^6*g2^3) + (2*t^7.18)/(g1^4*g2^2) + (4*t^7.19)/(g1^2*g2) + 5*t^7.2 + 4*g1^2*g2*t^7.21 + 3*g1^4*g2^2*t^7.22 + g1^6*g2^3*t^7.23 + t^7.29/(g1^5*g2^4) + t^7.3/(g1^3*g2^3) - t^7.31/(g1*g2^2) + g1^3*t^7.33 + t^7.39/(g1^6*g2^6) + 6*g1^3*g2^6*t^8.08 + 5*g2^3*t^8.18 + 11*g1^2*g2^4*t^8.19 + 5*g1^4*g2^5*t^8.2 + (3*t^8.27)/g1^3 + (7*g2*t^8.28)/g1 + g1*g2^2*t^8.29 + 9*g1^3*g2^3*t^8.3 + 3*g1^5*g2^4*t^8.31 + t^8.37/(g1^6*g2^3) + (3*t^8.38)/(g1^4*g2^2) + 3*t^8.4 - g1^2*g2*t^8.41 + 4*g1^4*g2^2*t^8.42 + g1^6*g2^3*t^8.43 + t^8.5/(g1^3*g2^3) - (2*t^8.51)/(g1*g2^2) - (g1*t^8.52)/g2 - g1^3*t^8.53 - t^8.6/(g1^4*g2^5) - t^4.2/y - t^5.4/y - (2*g1*g2^2*t^6.49)/y - t^6.59/(g1^2*g2*y) - (g1^2*g2*t^6.61)/y + (g1^2*g2^4*t^7.59)/y + (2*g2*t^7.68)/(g1*y) - (3*g1*g2^2*t^7.69)/y + (2*g1^3*g2^3*t^7.7)/y - t^7.79/(g1^2*g2*y) - (g1^2*g2*t^7.81)/y + t^7.91/(g1*g2^2*y) + (g1^2*g2^4*t^8.79)/y + (2*g2*t^8.88)/(g1*y) + (2*g1*g2^2*t^8.89)/y + (2*g1^3*g2^3*t^8.9)/y + t^8.99/(g1^2*g2*y) - t^4.2*y - t^5.4*y - 2*g1*g2^2*t^6.49*y - (t^6.59*y)/(g1^2*g2) - g1^2*g2*t^6.61*y + g1^2*g2^4*t^7.59*y + (2*g2*t^7.68*y)/g1 - 3*g1*g2^2*t^7.69*y + 2*g1^3*g2^3*t^7.7*y - (t^7.79*y)/(g1^2*g2) - g1^2*g2*t^7.81*y + (t^7.91*y)/(g1*g2^2) + g1^2*g2^4*t^8.79*y + (2*g2*t^8.88*y)/g1 + 2*g1*g2^2*t^8.89*y + 2*g1^3*g2^3*t^8.9*y + (t^8.99*y)/(g1^2*g2) |
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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58451 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ | 1.4105 | 1.6615 | 0.8489 | [X:[], M:[0.7838, 1.2], q:[0.4098, 0.3951], qb:[0.4065, 0.3887], phi:[0.4]] | 2*t^2.35 + 2*t^2.4 + t^2.45 + t^3.55 + 4*t^3.6 + 3*t^4.7 + 4*t^4.75 + 2*t^4.76 + t^4.79 + 7*t^4.8 + t^4.81 + 2*t^4.84 + 2*t^4.85 + t^4.9 + 2*t^5.9 + 7*t^5.95 + 2*t^5.96 + t^5.99 + 5*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail |