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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55503 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ | 0.6477 | 0.8502 | 0.7618 | [M:[1.0, 0.919, 0.7196, 0.7196, 0.7601, 1.0405], q:[0.7601, 0.2399], qb:[0.5203, 0.5608], phi:[0.4797]] | [M:[[0], [-8], [-3], [-3], [1], [4]], q:[[1], [-1]], qb:[[2], [6]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }M_{4}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{4}$ | ${}M_{6}\phi_{1}^{2}$ | -2 | 2*t^2.159 + 2*t^2.28 + t^2.402 + t^2.757 + t^2.878 + t^3. + t^3.122 + t^3.963 + 3*t^4.318 + 4*t^4.439 + 6*t^4.561 + 3*t^4.682 + 2*t^4.804 + 2*t^4.916 + 3*t^5.037 + 4*t^5.159 + 5*t^5.28 + 3*t^5.402 + t^5.514 + t^5.523 + t^5.635 + 2*t^5.757 - 2*t^6. + t^6.122 + 2*t^6.243 + t^6.365 + 3*t^6.477 + 4*t^6.598 + 9*t^6.72 + 9*t^6.841 + 8*t^6.963 + 3*t^7.075 + 5*t^7.084 + 5*t^7.196 + 2*t^7.206 + 8*t^7.318 + 10*t^7.439 + 9*t^7.561 + 2*t^7.673 + 7*t^7.682 + 3*t^7.794 + 3*t^7.804 + 5*t^7.916 + 2*t^7.925 + 3*t^8.037 - 4*t^8.159 + t^8.271 - 5*t^8.28 + t^8.392 - 3*t^8.402 + 2*t^8.514 + 2*t^8.523 + 5*t^8.635 + 2*t^8.645 + t^8.757 + 2*t^8.767 + 6*t^8.878 - t^4.439/y - (2*t^6.598)/y - t^6.72/y - t^7.196/y + t^7.318/y + (4*t^7.439)/y + (3*t^7.561)/y + (3*t^7.682)/y + (2*t^7.916)/y + (4*t^8.037)/y + (6*t^8.159)/y + (7*t^8.28)/y + (3*t^8.402)/y + t^8.523/y + t^8.635/y - (2*t^8.757)/y - t^4.439*y - 2*t^6.598*y - t^6.72*y - t^7.196*y + t^7.318*y + 4*t^7.439*y + 3*t^7.561*y + 3*t^7.682*y + 2*t^7.916*y + 4*t^8.037*y + 6*t^8.159*y + 7*t^8.28*y + 3*t^8.402*y + t^8.523*y + t^8.635*y - 2*t^8.757*y | (2*t^2.159)/g1^3 + 2*g1*t^2.28 + g1^5*t^2.402 + t^2.757/g1^8 + t^2.878/g1^4 + t^3. + g1^4*t^3.122 + g1^7*t^3.963 + (3*t^4.318)/g1^6 + (4*t^4.439)/g1^2 + 6*g1^2*t^4.561 + 3*g1^6*t^4.682 + 2*g1^10*t^4.804 + (2*t^4.916)/g1^11 + (3*t^5.037)/g1^7 + (4*t^5.159)/g1^3 + 5*g1*t^5.28 + 3*g1^5*t^5.402 + t^5.514/g1^16 + g1^9*t^5.523 + t^5.635/g1^12 + (2*t^5.757)/g1^8 - 2*t^6. + g1^4*t^6.122 + 2*g1^8*t^6.243 + g1^12*t^6.365 + (3*t^6.477)/g1^9 + (4*t^6.598)/g1^5 + (9*t^6.72)/g1 + 9*g1^3*t^6.841 + 8*g1^7*t^6.963 + (3*t^7.075)/g1^14 + 5*g1^11*t^7.084 + (5*t^7.196)/g1^10 + 2*g1^15*t^7.206 + (8*t^7.318)/g1^6 + (10*t^7.439)/g1^2 + 9*g1^2*t^7.561 + (2*t^7.673)/g1^19 + 7*g1^6*t^7.682 + (3*t^7.794)/g1^15 + 3*g1^10*t^7.804 + (5*t^7.916)/g1^11 + 2*g1^14*t^7.925 + (3*t^8.037)/g1^7 - (4*t^8.159)/g1^3 + t^8.271/g1^24 - 5*g1*t^8.28 + t^8.392/g1^20 - 3*g1^5*t^8.402 + (2*t^8.514)/g1^16 + 2*g1^9*t^8.523 + (5*t^8.635)/g1^12 + 2*g1^13*t^8.645 + t^8.757/g1^8 + 2*g1^17*t^8.767 + (6*t^8.878)/g1^4 - t^4.439/(g1^2*y) - (2*t^6.598)/(g1^5*y) - t^6.72/(g1*y) - t^7.196/(g1^10*y) + t^7.318/(g1^6*y) + (4*t^7.439)/(g1^2*y) + (3*g1^2*t^7.561)/y + (3*g1^6*t^7.682)/y + (2*t^7.916)/(g1^11*y) + (4*t^8.037)/(g1^7*y) + (6*t^8.159)/(g1^3*y) + (7*g1*t^8.28)/y + (3*g1^5*t^8.402)/y + (g1^9*t^8.523)/y + t^8.635/(g1^12*y) - (2*t^8.757)/(g1^8*y) - (t^4.439*y)/g1^2 - (2*t^6.598*y)/g1^5 - (t^6.72*y)/g1 - (t^7.196*y)/g1^10 + (t^7.318*y)/g1^6 + (4*t^7.439*y)/g1^2 + 3*g1^2*t^7.561*y + 3*g1^6*t^7.682*y + (2*t^7.916*y)/g1^11 + (4*t^8.037*y)/g1^7 + (6*t^8.159*y)/g1^3 + 7*g1*t^8.28*y + 3*g1^5*t^8.402*y + g1^9*t^8.523*y + (t^8.635*y)/g1^12 - (2*t^8.757*y)/g1^8 |
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 |
---|---|---|---|---|---|---|---|---|---|
48124 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6522 | 0.858 | 0.7602 | [M:[1.0, 0.8868, 0.7076, 0.7076, 0.7641], q:[0.7641, 0.2359], qb:[0.5283, 0.5849], phi:[0.4717]] | 2*t^2.123 + 2*t^2.292 + t^2.462 + t^2.66 + 2*t^2.83 + t^3. + t^4.047 + 3*t^4.245 + 4*t^4.415 + 6*t^4.585 + 3*t^4.755 + 2*t^4.783 + 2*t^4.924 + 5*t^4.953 + 6*t^5.123 + 4*t^5.292 + t^5.321 + t^5.462 + 2*t^5.491 + 4*t^5.66 - 3*t^6. - t^4.415/y - t^4.415*y | detail |