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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57090 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{7}$ | 0.6434 | 0.8452 | 0.7613 | [M:[1.0, 0.9755, 0.7347, 1.0122, 0.7469, 0.7469, 1.0245], q:[0.7531, 0.2469], qb:[0.5122, 0.5122], phi:[0.4939]] | [M:[[0], [-8], [-5], [4], [-1], [-1], [8]], q:[[1], [-1]], qb:[[4], [4]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }M_{5}$, ${ }M_{6}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{4}$, ${ }M_{7}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{6}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$ | ${}M_{4}\phi_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$ | -3 | t^2.204 + 2*t^2.241 + 2*t^2.278 + t^2.963 + t^3. + t^3.037 + t^3.073 + t^3.796 + t^4.408 + 2*t^4.445 + 5*t^4.482 + 4*t^4.518 + 6*t^4.555 + t^5.167 + t^5.204 + 5*t^5.241 + 5*t^5.278 + 4*t^5.314 + 2*t^5.351 + t^5.927 - 3*t^6. + 3*t^6.037 + 3*t^6.073 + t^6.11 + t^6.147 + t^6.612 + 2*t^6.649 + 3*t^6.686 + 6*t^6.722 + 9*t^6.759 + 9*t^6.796 + 9*t^6.833 + t^6.869 + t^7.371 + t^7.408 + 4*t^7.445 + 4*t^7.482 + 12*t^7.518 + 11*t^7.555 + 8*t^7.592 + 6*t^7.629 + t^8.131 - 3*t^8.204 - 7*t^8.241 - 4*t^8.278 + 5*t^8.314 + 9*t^8.351 + 4*t^8.388 + 2*t^8.425 + t^8.816 + 2*t^8.853 + 4*t^8.89 + 5*t^8.927 + 5*t^8.963 - t^4.482/y - t^6.686/y - (2*t^6.722)/y + (2*t^7.445)/y + (3*t^7.482)/y + (4*t^7.518)/y + t^7.555/y + t^8.167/y + (3*t^8.204)/y + (7*t^8.241)/y + (6*t^8.278)/y + (4*t^8.314)/y + (2*t^8.351)/y - t^8.89/y - (2*t^8.927)/y - (2*t^8.963)/y - t^4.482*y - t^6.686*y - 2*t^6.722*y + 2*t^7.445*y + 3*t^7.482*y + 4*t^7.518*y + t^7.555*y + t^8.167*y + 3*t^8.204*y + 7*t^8.241*y + 6*t^8.278*y + 4*t^8.314*y + 2*t^8.351*y - t^8.89*y - 2*t^8.927*y - 2*t^8.963*y | t^2.204/g1^5 + (2*t^2.241)/g1 + 2*g1^3*t^2.278 + t^2.963/g1^4 + t^3. + g1^4*t^3.037 + g1^8*t^3.073 + g1^5*t^3.796 + t^4.408/g1^10 + (2*t^4.445)/g1^6 + (5*t^4.482)/g1^2 + 4*g1^2*t^4.518 + 6*g1^6*t^4.555 + t^5.167/g1^9 + t^5.204/g1^5 + (5*t^5.241)/g1 + 5*g1^3*t^5.278 + 4*g1^7*t^5.314 + 2*g1^11*t^5.351 + t^5.927/g1^8 - 3*t^6. + 3*g1^4*t^6.037 + 3*g1^8*t^6.073 + g1^12*t^6.11 + g1^16*t^6.147 + t^6.612/g1^15 + (2*t^6.649)/g1^11 + (3*t^6.686)/g1^7 + (6*t^6.722)/g1^3 + 9*g1*t^6.759 + 9*g1^5*t^6.796 + 9*g1^9*t^6.833 + g1^13*t^6.869 + t^7.371/g1^14 + t^7.408/g1^10 + (4*t^7.445)/g1^6 + (4*t^7.482)/g1^2 + 12*g1^2*t^7.518 + 11*g1^6*t^7.555 + 8*g1^10*t^7.592 + 6*g1^14*t^7.629 + t^8.131/g1^13 - (3*t^8.204)/g1^5 - (7*t^8.241)/g1 - 4*g1^3*t^8.278 + 5*g1^7*t^8.314 + 9*g1^11*t^8.351 + 4*g1^15*t^8.388 + 2*g1^19*t^8.425 + t^8.816/g1^20 + (2*t^8.853)/g1^16 + (4*t^8.89)/g1^12 + (5*t^8.927)/g1^8 + (5*t^8.963)/g1^4 - t^4.482/(g1^2*y) - t^6.686/(g1^7*y) - (2*t^6.722)/(g1^3*y) + (2*t^7.445)/(g1^6*y) + (3*t^7.482)/(g1^2*y) + (4*g1^2*t^7.518)/y + (g1^6*t^7.555)/y + t^8.167/(g1^9*y) + (3*t^8.204)/(g1^5*y) + (7*t^8.241)/(g1*y) + (6*g1^3*t^8.278)/y + (4*g1^7*t^8.314)/y + (2*g1^11*t^8.351)/y - t^8.89/(g1^12*y) - (2*t^8.927)/(g1^8*y) - (2*t^8.963)/(g1^4*y) - (t^4.482*y)/g1^2 - (t^6.686*y)/g1^7 - (2*t^6.722*y)/g1^3 + (2*t^7.445*y)/g1^6 + (3*t^7.482*y)/g1^2 + 4*g1^2*t^7.518*y + g1^6*t^7.555*y + (t^8.167*y)/g1^9 + (3*t^8.204*y)/g1^5 + (7*t^8.241*y)/g1 + 6*g1^3*t^8.278*y + 4*g1^7*t^8.314*y + 2*g1^11*t^8.351*y - (t^8.89*y)/g1^12 - (2*t^8.927*y)/g1^8 - (2*t^8.963*y)/g1^4 |
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 |
---|---|---|---|---|---|---|---|---|---|
55490 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.6491 | 0.853 | 0.761 | [M:[1.0, 0.9038, 0.6899, 1.0481, 0.738, 0.738], q:[0.762, 0.238], qb:[0.5481, 0.5481], phi:[0.476]] | t^2.07 + 2*t^2.214 + 2*t^2.358 + t^2.711 + t^2.856 + t^3. + t^3.144 + t^3.93 + t^4.139 + 2*t^4.284 + 5*t^4.428 + 4*t^4.572 + 6*t^4.716 + t^4.781 + 3*t^4.925 + 3*t^5.07 + 5*t^5.214 + 4*t^5.358 + t^5.423 + 2*t^5.502 + t^5.567 + 2*t^5.711 + t^5.856 - 3*t^6. - t^4.428/y - t^4.428*y | detail |