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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2881 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}X_{1}$ + ${ }M_{2}M_{6}$ | 0.6497 | 0.8094 | 0.8027 | [X:[1.6113], M:[0.7774, 1.166, 0.3887, 0.834, 0.7774, 0.834], q:[0.4453, 0.7774], qb:[0.3887, 0.834], phi:[0.3887]] | [X:[[1]], M:[[-2], [-3], [-1], [3], [-2], [3]], q:[[4], [-2]], qb:[[-1], [3]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ | ${}M_{5}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ | 0 | 3*t^2.332 + 2*t^2.502 + t^3.498 + t^3.668 + 2*t^3.838 + 6*t^4.664 + 7*t^4.834 + 3*t^5.004 + t^5.83 + 6*t^6.17 + 4*t^6.34 + 9*t^6.996 + 10*t^7.166 + 7*t^7.336 + 4*t^7.506 + 3*t^7.676 - 7*t^8.332 + 2*t^8.502 + 11*t^8.672 + 6*t^8.842 - t^4.166/y - (3*t^6.498)/y - t^6.668/y + (4*t^7.664)/y + (9*t^7.834)/y + t^8.004/y - (3*t^8.83)/y - t^4.166*y - 3*t^6.498*y - t^6.668*y + 4*t^7.664*y + 9*t^7.834*y + t^8.004*y - 3*t^8.83*y | (3*t^2.332)/g1^2 + 2*g1^3*t^2.502 + t^3.498/g1^3 + g1^2*t^3.668 + 2*g1^7*t^3.838 + (6*t^4.664)/g1^4 + 7*g1*t^4.834 + 3*g1^6*t^5.004 + t^5.83/g1^5 + 6*g1^5*t^6.17 + 4*g1^10*t^6.34 + (9*t^6.996)/g1^6 + (10*t^7.166)/g1 + 7*g1^4*t^7.336 + 4*g1^9*t^7.506 + 3*g1^14*t^7.676 - (7*t^8.332)/g1^2 + 2*g1^3*t^8.502 + 11*g1^8*t^8.672 + 6*g1^13*t^8.842 - t^4.166/(g1*y) - (3*t^6.498)/(g1^3*y) - (g1^2*t^6.668)/y + (4*t^7.664)/(g1^4*y) + (9*g1*t^7.834)/y + (g1^6*t^8.004)/y - (3*t^8.83)/(g1^5*y) - (t^4.166*y)/g1 - (3*t^6.498*y)/g1^3 - g1^2*t^6.668*y + (4*t^7.664*y)/g1^4 + 9*g1*t^7.834*y + g1^6*t^8.004*y - (3*t^8.83*y)/g1^5 |
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 |
---|---|---|---|---|---|---|---|---|---|
1868 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}X_{1}$ | 0.6359 | 0.7849 | 0.8102 | [X:[1.616], M:[0.7681, 1.1521, 0.384, 0.8479, 0.7681], q:[0.4639, 0.7681], qb:[0.384, 0.8479], phi:[0.384]] | 3*t^2.304 + t^2.544 + 2*t^3.456 + t^3.696 + 2*t^3.935 + 6*t^4.608 + 4*t^4.848 + t^5.087 + 4*t^5.761 - t^4.152/y - t^4.152*y | detail |