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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5636 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{3}M_{7}$ + ${ }M_{2}M_{8}$ + ${ }M_{9}q_{1}q_{2}$ | 0.7021 | 0.895 | 0.7845 | [M:[1.0132, 1.0729, 1.1589, 0.8411, 0.6953, 0.9868, 0.8411, 0.9271, 0.6953], q:[0.7682, 0.5364], qb:[0.4504, 0.3907], phi:[0.4636]] | [M:[[13], [-4], [5], [-5], [3], [-13], [-5], [4], [3]], q:[[-1], [-2]], qb:[[-11], [6]], phi:[[2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{5}$, ${ }M_{9}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{9}$, ${ }M_{9}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{4}M_{9}$, ${ }M_{7}M_{9}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{8}M_{9}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{9}\phi_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{6}M_{9}$, ${ }M_{4}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{8}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{6}M_{8}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{1}$, ${ }M_{9}q_{1}\tilde{q}_{1}$, ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{9}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{6}^{2}$ | ${}$ | -3 | 2*t^2.086 + 2*t^2.523 + 2*t^2.781 + t^2.961 + t^3.656 + t^3.735 + t^4.093 + 4*t^4.172 + t^4.351 + 5*t^4.609 + 4*t^4.867 + 5*t^5.047 + 4*t^5.305 + 2*t^5.484 + 2*t^5.563 + 3*t^5.742 + t^5.821 + t^5.921 - 3*t^6. + 3*t^6.179 + 6*t^6.258 + t^6.437 + 2*t^6.516 + 3*t^6.616 + 8*t^6.695 + 3*t^6.874 + 5*t^6.953 + t^7.054 + 10*t^7.133 - t^7.212 + t^7.312 + 7*t^7.391 + t^7.47 + 6*t^7.57 + 2*t^7.649 + t^7.749 + 8*t^7.828 + 2*t^7.907 + 5*t^8.007 - 4*t^8.086 + t^8.186 + 6*t^8.265 + 9*t^8.344 + 3*t^8.444 - 6*t^8.523 + 2*t^8.602 + 9*t^8.702 + 5*t^8.781 + t^8.882 - t^4.391/y - (2*t^6.477)/y - t^6.914/y + (5*t^7.609)/y + (5*t^7.867)/y + (3*t^8.047)/y + (6*t^8.305)/y + (2*t^8.484)/y - (2*t^8.563)/y + (4*t^8.742)/y + (2*t^8.821)/y - t^4.391*y - 2*t^6.477*y - t^6.914*y + 5*t^7.609*y + 5*t^7.867*y + 3*t^8.047*y + 6*t^8.305*y + 2*t^8.484*y - 2*t^8.563*y + 4*t^8.742*y + 2*t^8.821*y | 2*g1^3*t^2.086 + (2*t^2.523)/g1^5 + 2*g1^4*t^2.781 + t^2.961/g1^13 + t^3.656/g1^12 + g1^14*t^3.735 + t^4.093/g1^20 + 4*g1^6*t^4.172 + t^4.351/g1^11 + (5*t^4.609)/g1^2 + 4*g1^7*t^4.867 + (5*t^5.047)/g1^10 + (4*t^5.305)/g1 + (2*t^5.484)/g1^18 + 2*g1^8*t^5.563 + (3*t^5.742)/g1^9 + g1^17*t^5.821 + t^5.921/g1^26 - 3*t^6. + (3*t^6.179)/g1^17 + 6*g1^9*t^6.258 + t^6.437/g1^8 + 2*g1^18*t^6.516 + (3*t^6.616)/g1^25 + 8*g1*t^6.695 + (3*t^6.874)/g1^16 + 5*g1^10*t^6.953 + t^7.054/g1^33 + (10*t^7.133)/g1^7 - g1^19*t^7.212 + t^7.312/g1^24 + 7*g1^2*t^7.391 + g1^28*t^7.47 + (6*t^7.57)/g1^15 + 2*g1^11*t^7.649 + t^7.749/g1^32 + (8*t^7.828)/g1^6 + 2*g1^20*t^7.907 + (5*t^8.007)/g1^23 - 4*g1^3*t^8.086 + t^8.186/g1^40 + (6*t^8.265)/g1^14 + 9*g1^12*t^8.344 + (3*t^8.444)/g1^31 - (6*t^8.523)/g1^5 + 2*g1^21*t^8.602 + (9*t^8.702)/g1^22 + 5*g1^4*t^8.781 + t^8.882/g1^39 - (g1^2*t^4.391)/y - (2*g1^5*t^6.477)/y - t^6.914/(g1^3*y) + (5*t^7.609)/(g1^2*y) + (5*g1^7*t^7.867)/y + (3*t^8.047)/(g1^10*y) + (6*t^8.305)/(g1*y) + (2*t^8.484)/(g1^18*y) - (2*g1^8*t^8.563)/y + (4*t^8.742)/(g1^9*y) + (2*g1^17*t^8.821)/y - g1^2*t^4.391*y - 2*g1^5*t^6.477*y - (t^6.914*y)/g1^3 + (5*t^7.609*y)/g1^2 + 5*g1^7*t^7.867*y + (3*t^8.047*y)/g1^10 + (6*t^8.305*y)/g1 + (2*t^8.484*y)/g1^18 - 2*g1^8*t^8.563*y + (4*t^8.742*y)/g1^9 + 2*g1^17*t^8.821*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 |
---|---|---|---|---|---|---|---|---|---|
4137 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{3}M_{7}$ + ${ }M_{2}M_{8}$ | 0.6815 | 0.8555 | 0.7967 | [M:[1.015, 1.0723, 1.1596, 0.8404, 0.6958, 0.985, 0.8404, 0.9277], q:[0.7681, 0.5362], qb:[0.4488, 0.3915], phi:[0.4638]] | t^2.087 + 2*t^2.521 + 2*t^2.783 + t^2.955 + t^3.651 + t^3.741 + t^3.913 + t^4.085 + 2*t^4.175 + t^4.347 + 3*t^4.608 + 2*t^4.87 + 4*t^5.042 + 4*t^5.304 + 2*t^5.476 + 2*t^5.566 + 2*t^5.738 + t^5.91 - 2*t^6. - t^4.392/y - t^4.392*y | detail |