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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4117 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{7}q_{1}\tilde{q}_{2}$ + ${ }M_{8}q_{1}\tilde{q}_{1}$ | 0.7162 | 0.9094 | 0.7876 | [M:[1.0906, 1.0906, 1.0015, 0.9094, 0.7251, 0.9094, 0.7281, 0.7281], q:[0.7727, 0.4101], qb:[0.4993, 0.4993], phi:[0.4547]] | [M:[[4], [4], [-22], [-4], [32], [-4], [-12], [-12]], q:[[1], [-15]], qb:[[11], [11]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{5}$, ${ }M_{7}$, ${ }M_{8}$, ${ }M_{4}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{5}M_{8}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{7}^{2}$, ${ }M_{7}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{6}M_{8}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{7}$, ${ }M_{3}M_{8}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{5}q_{1}q_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{7}q_{1}q_{2}$, ${ }M_{8}q_{1}q_{2}$ | ${}$ | -5 | t^2.175 + 2*t^2.184 + 3*t^2.728 + t^3.004 + t^3.548 + 2*t^4.092 + t^4.351 + 5*t^4.36 + 3*t^4.368 + 3*t^4.903 + 6*t^4.912 + t^5.18 + 2*t^5.189 + 6*t^5.456 + t^5.724 + 3*t^5.733 - 5*t^6. + t^6.009 + 6*t^6.276 + t^6.526 + 5*t^6.535 + 6*t^6.544 + 5*t^6.553 + 3*t^6.82 + 3*t^7.079 + 12*t^7.088 + 9*t^7.097 + t^7.355 - t^7.364 + 3*t^7.373 + t^7.632 + 12*t^7.64 + t^7.899 + 2*t^7.908 + 5*t^7.917 - 7*t^8.175 + 2*t^8.193 + 4*t^8.452 + 10*t^8.461 + t^8.701 + 5*t^8.71 + 11*t^8.719 - 7*t^8.728 + 8*t^8.737 - 3*t^8.996 - t^4.364/y - t^6.539/y - (2*t^6.548)/y - t^7.092/y + (3*t^7.36)/y + t^7.636/y + (3*t^7.903)/y + (6*t^7.912)/y + (3*t^8.18)/y + (3*t^8.189)/y + (3*t^8.456)/y - t^8.715/y - t^8.724/y + (2*t^8.733)/y - t^4.364*y - t^6.539*y - 2*t^6.548*y - t^7.092*y + 3*t^7.36*y + t^7.636*y + 3*t^7.903*y + 6*t^7.912*y + 3*t^8.18*y + 3*t^8.189*y + 3*t^8.456*y - t^8.715*y - t^8.724*y + 2*t^8.733*y | g1^32*t^2.175 + (2*t^2.184)/g1^12 + (3*t^2.728)/g1^4 + t^3.004/g1^22 + t^3.548/g1^14 + (2*t^4.092)/g1^6 + g1^64*t^4.351 + 5*g1^20*t^4.36 + (3*t^4.368)/g1^24 + 3*g1^28*t^4.903 + (6*t^4.912)/g1^16 + g1^10*t^5.18 + (2*t^5.189)/g1^34 + (6*t^5.456)/g1^8 + g1^18*t^5.724 + (3*t^5.733)/g1^26 - 5*t^6. + t^6.009/g1^44 + (6*t^6.276)/g1^18 + g1^96*t^6.526 + 5*g1^52*t^6.535 + 6*g1^8*t^6.544 + (5*t^6.553)/g1^36 + (3*t^6.82)/g1^10 + 3*g1^60*t^7.079 + 12*g1^16*t^7.088 + (9*t^7.097)/g1^28 + g1^42*t^7.355 - t^7.364/g1^2 + (3*t^7.373)/g1^46 + g1^24*t^7.632 + (12*t^7.64)/g1^20 + g1^50*t^7.899 + 2*g1^6*t^7.908 + (5*t^7.917)/g1^38 - 7*g1^32*t^8.175 + (2*t^8.193)/g1^56 + 4*g1^14*t^8.452 + (10*t^8.461)/g1^30 + g1^128*t^8.701 + 5*g1^84*t^8.71 + 11*g1^40*t^8.719 - (7*t^8.728)/g1^4 + (8*t^8.737)/g1^48 - 3*g1^22*t^8.996 - t^4.364/(g1^2*y) - (g1^30*t^6.539)/y - (2*t^6.548)/(g1^14*y) - t^7.092/(g1^6*y) + (3*g1^20*t^7.36)/y + (g1^2*t^7.636)/y + (3*g1^28*t^7.903)/y + (6*t^7.912)/(g1^16*y) + (3*g1^10*t^8.18)/y + (3*t^8.189)/(g1^34*y) + (3*t^8.456)/(g1^8*y) - (g1^62*t^8.715)/y - (g1^18*t^8.724)/y + (2*t^8.733)/(g1^26*y) - (t^4.364*y)/g1^2 - g1^30*t^6.539*y - (2*t^6.548*y)/g1^14 - (t^7.092*y)/g1^6 + 3*g1^20*t^7.36*y + g1^2*t^7.636*y + 3*g1^28*t^7.903*y + (6*t^7.912*y)/g1^16 + 3*g1^10*t^8.18*y + (3*t^8.189*y)/g1^34 + (3*t^8.456*y)/g1^8 - g1^62*t^8.715*y - g1^18*t^8.724*y + (2*t^8.733*y)/g1^26 |
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 |
---|---|---|---|---|---|---|---|---|---|
2143 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{7}q_{1}\tilde{q}_{2}$ | 0.6964 | 0.8727 | 0.798 | [M:[1.0896, 1.0896, 1.0073, 0.9104, 0.7166, 0.9104, 0.7313], q:[0.7724, 0.4141], qb:[0.4963, 0.4963], phi:[0.4552]] | t^2.15 + t^2.194 + 3*t^2.731 + t^3.022 + t^3.559 + t^3.806 + 2*t^4.097 + t^4.3 + 4*t^4.344 + t^4.388 + 3*t^4.881 + 3*t^4.925 + t^5.172 + t^5.216 + 6*t^5.463 + t^5.709 + 2*t^5.753 + t^5.956 - 4*t^6. - t^4.366/y - t^4.366*y | detail |