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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3111 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}M_{5}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{7}q_{1}\tilde{q}_{2}$ | 0.6255 | 0.8112 | 0.7711 | [M:[0.9857, 1.043, 0.9857, 0.7464, 1.2536, 0.7751, 0.7751], q:[0.7464, 0.2679], qb:[0.4785, 0.4785], phi:[0.5072]] | [M:[[4], [-12], [4], [1], [-1], [-7], [-7]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{6}$, ${ }M_{7}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }M_{7}q_{2}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$ | ${}M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | -2 | 2*t^2.239 + 2*t^2.325 + 2*t^2.957 + 2*t^3.129 + 2*t^3.761 + 3*t^4.392 + 3*t^4.478 + 4*t^4.565 + 3*t^4.651 + 4*t^5.196 + 4*t^5.282 + 2*t^5.368 + 4*t^5.454 + 2*t^5.914 - 2*t^6. + 6*t^6.086 + 3*t^6.258 + 2*t^6.632 + 10*t^6.718 + 2*t^6.804 + 8*t^6.89 + 4*t^6.976 + 3*t^7.349 + t^7.435 + 9*t^7.522 + 8*t^7.608 + 4*t^7.694 + 6*t^7.78 - 2*t^8.067 + 4*t^8.153 - 2*t^8.239 - 4*t^8.325 + 10*t^8.411 + 2*t^8.497 + 6*t^8.584 + 5*t^8.785 + 3*t^8.871 - 2*t^8.957 - t^4.522/y - (2*t^6.847)/y + t^7.392/y + (5*t^7.565)/y + (6*t^8.196)/y + (4*t^8.282)/y + (4*t^8.368)/y + (4*t^8.454)/y + t^8.914/y - t^4.522*y - 2*t^6.847*y + t^7.392*y + 5*t^7.565*y + 6*t^8.196*y + 4*t^8.282*y + 4*t^8.368*y + 4*t^8.454*y + t^8.914*y | 2*g1*t^2.239 + (2*t^2.325)/g1^7 + 2*g1^4*t^2.957 + (2*t^3.129)/g1^12 + (2*t^3.761)/g1 + 3*g1^10*t^4.392 + 3*g1^2*t^4.478 + (4*t^4.565)/g1^6 + (3*t^4.651)/g1^14 + 4*g1^5*t^5.196 + (4*t^5.282)/g1^3 + (2*t^5.368)/g1^11 + (4*t^5.454)/g1^19 + 2*g1^8*t^5.914 - 2*t^6. + (6*t^6.086)/g1^8 + (3*t^6.258)/g1^24 + 2*g1^11*t^6.632 + 10*g1^3*t^6.718 + (2*t^6.804)/g1^5 + (8*t^6.89)/g1^13 + (4*t^6.976)/g1^21 + 3*g1^14*t^7.349 + g1^6*t^7.435 + (9*t^7.522)/g1^2 + (8*t^7.608)/g1^10 + (4*t^7.694)/g1^18 + (6*t^7.78)/g1^26 - 2*g1^17*t^8.067 + 4*g1^9*t^8.153 - 2*g1*t^8.239 - (4*t^8.325)/g1^7 + (10*t^8.411)/g1^15 + (2*t^8.497)/g1^23 + (6*t^8.584)/g1^31 + 5*g1^20*t^8.785 + 3*g1^12*t^8.871 - 2*g1^4*t^8.957 - t^4.522/(g1^2*y) - (2*t^6.847)/(g1^9*y) + (g1^10*t^7.392)/y + (5*t^7.565)/(g1^6*y) + (6*g1^5*t^8.196)/y + (4*t^8.282)/(g1^3*y) + (4*t^8.368)/(g1^11*y) + (4*t^8.454)/(g1^19*y) + (g1^8*t^8.914)/y - (t^4.522*y)/g1^2 - (2*t^6.847*y)/g1^9 + g1^10*t^7.392*y + (5*t^7.565*y)/g1^6 + 6*g1^5*t^8.196*y + (4*t^8.282*y)/g1^3 + (4*t^8.368*y)/g1^11 + (4*t^8.454*y)/g1^19 + g1^8*t^8.914*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 |
---|---|---|---|---|---|---|---|---|---|
2040 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}M_{5}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ | 0.6079 | 0.7795 | 0.7799 | [M:[0.9787, 1.0638, 0.9787, 0.7447, 1.2553, 0.7872], q:[0.7447, 0.2766], qb:[0.4681, 0.4681], phi:[0.5106]] | 2*t^2.234 + t^2.362 + 2*t^2.936 + 2*t^3.192 + t^3.638 + 2*t^3.766 + 3*t^4.34 + 3*t^4.468 + 2*t^4.596 + t^4.723 + 4*t^5.17 + 2*t^5.298 + 2*t^5.426 + 2*t^5.553 + 4*t^5.872 - t^6. - t^4.532/y - t^4.532*y | detail |