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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4630 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{5}M_{7}$ + ${ }M_{6}M_{8}$ | 0.6979 | 0.862 | 0.8097 | [M:[1.0835, 0.7496, 0.874, 0.9591, 1.0409, 0.7922, 0.9591, 1.2078], q:[0.5417, 0.3748], qb:[0.5843, 0.6661], phi:[0.4583]] | [M:[[-2], [6], [15], [-11], [11], [-7], [-11], [7]], q:[[-1], [3]], qb:[[-14], [8]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{1}$, ${ }M_{8}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{8}$ | ${}$ | -3 | t^2.249 + t^2.622 + t^2.75 + 2*t^2.877 + t^3.25 + 2*t^3.624 + t^4.124 + t^4.252 + 2*t^4.497 + t^4.625 + t^4.753 + t^4.871 + t^4.881 + 2*t^4.998 + 2*t^5.126 + t^5.244 + t^5.371 + 3*t^5.499 + t^5.627 + 2*t^5.755 + 2*t^5.872 - 3*t^6. + t^6.128 + t^6.245 + 2*t^6.373 + 3*t^6.501 - t^6.629 + 2*t^6.746 + 2*t^6.874 + 2*t^7.002 + 2*t^7.119 + 2*t^7.129 + 5*t^7.247 + 2*t^7.375 + t^7.492 + 2*t^7.503 + t^7.62 + 2*t^7.63 + 4*t^7.748 + 2*t^7.758 + t^7.866 + t^7.876 + t^7.993 + t^8.003 + 5*t^8.121 - t^8.249 + 3*t^8.376 + 2*t^8.494 + 2*t^8.504 + 2*t^8.632 + t^8.867 - 6*t^8.877 + 3*t^8.995 - t^4.375/y - t^6.624/y - t^6.997/y - t^7.252/y + t^7.497/y + t^7.753/y + t^7.871/y + t^7.998/y + (3*t^8.126)/y + t^8.371/y + (3*t^8.499)/y + (2*t^8.627)/y + t^8.755/y + (2*t^8.872)/y - t^4.375*y - t^6.624*y - t^6.997*y - t^7.252*y + t^7.497*y + t^7.753*y + t^7.871*y + t^7.998*y + 3*t^8.126*y + t^8.371*y + 3*t^8.499*y + 2*t^8.627*y + t^8.755*y + 2*t^8.872*y | g1^6*t^2.249 + g1^15*t^2.622 + g1^2*t^2.75 + (2*t^2.877)/g1^11 + t^3.25/g1^2 + 2*g1^7*t^3.624 + g1^3*t^4.124 + t^4.252/g1^10 + 2*g1^12*t^4.497 + t^4.625/g1 + t^4.753/g1^14 + g1^21*t^4.871 + t^4.881/g1^27 + 2*g1^8*t^4.998 + (2*t^5.126)/g1^5 + g1^30*t^5.244 + g1^17*t^5.371 + 3*g1^4*t^5.499 + t^5.627/g1^9 + (2*t^5.755)/g1^22 + 2*g1^13*t^5.872 - 3*t^6. + t^6.128/g1^13 + g1^22*t^6.245 + 2*g1^9*t^6.373 + (3*t^6.501)/g1^4 - t^6.629/g1^17 + 2*g1^18*t^6.746 + 2*g1^5*t^6.874 + (2*t^7.002)/g1^8 + 2*g1^27*t^7.119 + (2*t^7.129)/g1^21 + 5*g1^14*t^7.247 + 2*g1*t^7.375 + g1^36*t^7.492 + (2*t^7.503)/g1^12 + g1^23*t^7.62 + (2*t^7.63)/g1^25 + 4*g1^10*t^7.748 + (2*t^7.758)/g1^38 + g1^45*t^7.866 + t^7.876/g1^3 + g1^32*t^7.993 + t^8.003/g1^16 + 5*g1^19*t^8.121 - g1^6*t^8.249 + (3*t^8.376)/g1^7 + 2*g1^28*t^8.494 + (2*t^8.504)/g1^20 + (2*t^8.632)/g1^33 + g1^37*t^8.867 - (6*t^8.877)/g1^11 + 3*g1^24*t^8.995 - (g1*t^4.375)/y - (g1^7*t^6.624)/y - (g1^16*t^6.997)/y - t^7.252/(g1^10*y) + (g1^12*t^7.497)/y + t^7.753/(g1^14*y) + (g1^21*t^7.871)/y + (g1^8*t^7.998)/y + (3*t^8.126)/(g1^5*y) + (g1^17*t^8.371)/y + (3*g1^4*t^8.499)/y + (2*t^8.627)/(g1^9*y) + t^8.755/(g1^22*y) + (2*g1^13*t^8.872)/y - g1*t^4.375*y - g1^7*t^6.624*y - g1^16*t^6.997*y - (t^7.252*y)/g1^10 + g1^12*t^7.497*y + (t^7.753*y)/g1^14 + g1^21*t^7.871*y + g1^8*t^7.998*y + (3*t^8.126*y)/g1^5 + g1^17*t^8.371*y + 3*g1^4*t^8.499*y + (2*t^8.627*y)/g1^9 + (t^8.755*y)/g1^22 + 2*g1^13*t^8.872*y |
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 |
---|---|---|---|---|---|---|---|---|---|
2555 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{5}M_{7}$ | 0.7151 | 0.8924 | 0.8013 | [M:[1.0817, 0.7548, 0.887, 0.9495, 1.0505, 0.7861, 0.9495], q:[0.5409, 0.3774], qb:[0.5721, 0.6731], phi:[0.4591]] | t^2.264 + t^2.358 + t^2.661 + t^2.755 + 2*t^2.849 + t^3.245 + t^3.642 + t^4.132 + t^4.226 + 2*t^4.529 + 2*t^4.623 + 2*t^4.716 + t^4.81 + t^4.926 + 3*t^5.019 + 3*t^5.113 + 2*t^5.207 + t^5.322 + t^5.416 + 3*t^5.51 + 2*t^5.603 + 2*t^5.697 + t^5.906 - 2*t^6. - t^4.377/y - t^4.377*y | detail |