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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58391 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$ | 1.3451 | 1.6131 | 0.8339 | [X:[], M:[0.7133], q:[0.5911, 0.4178], qb:[0.2956, 0.2956], phi:[0.4]] | [X:[], M:[[-3]], q:[[2], [-4]], qb:[[1], [1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ 2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ 2}\phi_{1}q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}^{3}$ | 8 | 3*t^2.14 + t^2.4 + 2*t^2.66 + 2*t^3.34 + t^3.6 + 3*t^3.86 + 6*t^4.28 + 5*t^4.54 + 7*t^4.8 + 6*t^5.06 + 3*t^5.32 + 6*t^5.48 + 5*t^5.74 + 8*t^6. + 9*t^6.26 + 10*t^6.42 + 4*t^6.52 + 15*t^6.68 + 17*t^6.94 + 20*t^7.2 + t^7.36 + 14*t^7.46 + 12*t^7.62 + 11*t^7.72 + 16*t^7.88 + 4*t^7.98 + 15*t^8.14 + 28*t^8.4 + 15*t^8.56 + 11*t^8.66 + 29*t^8.82 + 19*t^8.92 - t^4.2/y - t^5.4/y - (3*t^6.34)/y - t^6.6/y - (2*t^6.86)/y + (3*t^7.28)/y + (5*t^7.8)/y + t^8.06/y + t^8.32/y - t^4.2*y - t^5.4*y - 3*t^6.34*y - t^6.6*y - 2*t^6.86*y + 3*t^7.28*y + 5*t^7.8*y + t^8.06*y + t^8.32*y | (3*t^2.14)/g1^3 + t^2.4 + 2*g1^3*t^2.66 + (2*t^3.34)/g1^3 + t^3.6 + 3*g1^3*t^3.86 + (6*t^4.28)/g1^6 + (5*t^4.54)/g1^3 + 7*t^4.8 + 6*g1^3*t^5.06 + 3*g1^6*t^5.32 + (6*t^5.48)/g1^6 + (5*t^5.74)/g1^3 + 8*t^6. + 9*g1^3*t^6.26 + (10*t^6.42)/g1^9 + 4*g1^6*t^6.52 + (15*t^6.68)/g1^6 + (17*t^6.94)/g1^3 + 20*t^7.2 + t^7.36/g1^12 + 14*g1^3*t^7.46 + (12*t^7.62)/g1^9 + 11*g1^6*t^7.72 + (16*t^7.88)/g1^6 + 4*g1^9*t^7.98 + (15*t^8.14)/g1^3 + 28*t^8.4 + (15*t^8.56)/g1^12 + 11*g1^3*t^8.66 + (29*t^8.82)/g1^9 + 19*g1^6*t^8.92 - t^4.2/y - t^5.4/y - (3*t^6.34)/(g1^3*y) - t^6.6/y - (2*g1^3*t^6.86)/y + (3*t^7.28)/(g1^6*y) + (5*t^7.8)/y + (g1^3*t^8.06)/y + (g1^6*t^8.32)/y - t^4.2*y - t^5.4*y - (3*t^6.34*y)/g1^3 - t^6.6*y - 2*g1^3*t^6.86*y + (3*t^7.28*y)/g1^6 + 5*t^7.8*y + g1^3*t^8.06*y + g1^6*t^8.32*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 |
---|---|---|---|---|---|---|---|---|---|
57347 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ | 1.3452 | 1.6133 | 0.8338 | [M:[0.7103], q:[0.591, 0.4181], qb:[0.2987, 0.2923], phi:[0.4]] | 2*t^2.131 + t^2.15 + t^2.4 + t^2.65 + t^2.669 + t^3.331 + t^3.35 + t^3.6 + 2*t^3.85 + t^3.869 + 3*t^4.262 + 2*t^4.281 + t^4.301 + 3*t^4.531 + 2*t^4.55 + 2*t^4.781 + 4*t^4.8 + t^4.819 + 3*t^5.05 + 3*t^5.069 + t^5.299 + t^5.319 + t^5.338 + 2*t^5.462 + 3*t^5.481 + t^5.501 + 3*t^5.731 + 2*t^5.75 + 4*t^5.981 + 3*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail |