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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46651 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{4}$ | 0.6055 | 0.7768 | 0.7796 | [X:[], M:[0.9916, 0.7563, 1.0252, 1.0084], q:[0.7479, 0.2605], qb:[0.479, 0.4958], phi:[0.5042]] | [X:[], M:[[4], [-3], [-12], [-4]], q:[[1], [-5]], qb:[[10], [2]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$ | ${}M_{2}q_{1}\tilde{q}_{2}$ | -1 | t^2.22 + 2*t^2.27 + 2*t^3.03 + 2*t^3.08 + t^3.68 + t^3.73 + t^3.78 + t^4.39 + 2*t^4.44 + 3*t^4.49 + 3*t^4.54 + 2*t^5.24 + 5*t^5.29 + 3*t^5.34 + t^5.9 + t^5.95 - t^6. + 2*t^6.05 + 4*t^6.1 + 3*t^6.15 + t^6.6 + 2*t^6.66 + 3*t^6.71 + 5*t^6.76 + 5*t^6.81 + t^6.86 + t^7.41 + 2*t^7.46 + 5*t^7.51 + 8*t^7.56 + 4*t^7.61 + t^8.07 + 2*t^8.12 - 3*t^8.22 - 2*t^8.27 + 5*t^8.32 + 7*t^8.37 + 4*t^8.42 + t^8.77 + 2*t^8.82 + 3*t^8.87 + 3*t^8.92 + 2*t^8.97 - t^4.51/y - t^6.78/y + t^7.44/y + (3*t^7.49)/y - t^7.59/y + (3*t^8.24)/y + (6*t^8.29)/y + (4*t^8.34)/y + t^8.9/y + (3*t^8.95)/y - t^4.51*y - t^6.78*y + t^7.44*y + 3*t^7.49*y - t^7.59*y + 3*t^8.24*y + 6*t^8.29*y + 4*t^8.34*y + t^8.9*y + 3*t^8.95*y | g1^5*t^2.22 + (2*t^2.27)/g1^3 + (2*t^3.03)/g1^4 + (2*t^3.08)/g1^12 + g1^11*t^3.68 + g1^3*t^3.73 + t^3.78/g1^5 + g1^18*t^4.39 + 2*g1^10*t^4.44 + 3*g1^2*t^4.49 + (3*t^4.54)/g1^6 + 2*g1*t^5.24 + (5*t^5.29)/g1^7 + (3*t^5.34)/g1^15 + g1^16*t^5.9 + g1^8*t^5.95 - t^6. + (2*t^6.05)/g1^8 + (4*t^6.1)/g1^16 + (3*t^6.15)/g1^24 + g1^23*t^6.6 + 2*g1^15*t^6.66 + 3*g1^7*t^6.71 + (5*t^6.76)/g1 + (5*t^6.81)/g1^9 + t^6.86/g1^17 + g1^14*t^7.41 + 2*g1^6*t^7.46 + (5*t^7.51)/g1^2 + (8*t^7.56)/g1^10 + (4*t^7.61)/g1^18 + g1^29*t^8.07 + 2*g1^21*t^8.12 - 3*g1^5*t^8.22 - (2*t^8.27)/g1^3 + (5*t^8.32)/g1^11 + (7*t^8.37)/g1^19 + (4*t^8.42)/g1^27 + g1^36*t^8.77 + 2*g1^28*t^8.82 + 3*g1^20*t^8.87 + 3*g1^12*t^8.92 + 2*g1^4*t^8.97 - t^4.51/(g1^2*y) - t^6.78/(g1^5*y) + (g1^10*t^7.44)/y + (3*g1^2*t^7.49)/y - t^7.59/(g1^14*y) + (3*g1*t^8.24)/y + (6*t^8.29)/(g1^7*y) + (4*t^8.34)/(g1^15*y) + (g1^16*t^8.9)/y + (3*g1^8*t^8.95)/y - (t^4.51*y)/g1^2 - (t^6.78*y)/g1^5 + g1^10*t^7.44*y + 3*g1^2*t^7.49*y - (t^7.59*y)/g1^14 + 3*g1*t^8.24*y + (6*t^8.29*y)/g1^7 + (4*t^8.34*y)/g1^15 + g1^16*t^8.9*y + 3*g1^8*t^8.95*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 |
---|---|---|---|---|---|---|---|---|---|
46078 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6066 | 0.7783 | 0.7794 | [X:[], M:[0.9857, 0.7607, 1.043], q:[0.7464, 0.2679], qb:[0.4642, 0.4928], phi:[0.5072]] | t^2.2 + 2*t^2.28 + t^2.96 + t^3.04 + 2*t^3.13 + t^3.63 + t^3.72 + t^3.8 + t^4.31 + 2*t^4.39 + 3*t^4.48 + 3*t^4.56 + t^5.15 + 3*t^5.24 + 3*t^5.33 + 3*t^5.41 + t^5.83 + 2*t^5.91 - t^4.52/y - t^4.52*y | detail |