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 |
---|---|---|---|---|---|---|---|---|---|
46731 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{4}$ | 0.6453 | 0.804 | 0.8026 | [M:[0.8793, 1.2198, 0.7802, 0.7802], q:[0.681, 0.4397], qb:[0.3405, 0.7802], phi:[0.4397]] | [M:[[-4], [-1], [1], [1]], q:[[6], [-2]], qb:[[3], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{3}$, ${ }M_{4}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{3}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 2 | 2*t^2.34 + 2*t^2.638 + t^3.064 + 2*t^3.362 + t^3.66 + t^3.957 + 2*t^4.383 + 4*t^4.681 + 3*t^4.979 + 2*t^5.276 + 3*t^5.405 + 5*t^5.702 + 2*t^6. + t^6.129 + 2*t^6.426 + t^6.595 + 4*t^6.724 + 6*t^7.021 + 3*t^7.319 + 2*t^7.448 + 2*t^7.617 + 7*t^7.745 + 4*t^7.914 + 7*t^8.043 + 3*t^8.469 - 2*t^8.638 + 7*t^8.767 - 2*t^8.936 - t^4.319/y - t^6.66/y - (2*t^6.957)/y + (3*t^7.681)/y + (5*t^7.979)/y + t^8.276/y + (2*t^8.405)/y + (6*t^8.702)/y - t^4.319*y - t^6.66*y - 2*t^6.957*y + 3*t^7.681*y + 5*t^7.979*y + t^8.276*y + 2*t^8.405*y + 6*t^8.702*y | 2*g1*t^2.34 + (2*t^2.638)/g1^4 + g1^9*t^3.064 + 2*g1^4*t^3.362 + t^3.66/g1 + t^3.957/g1^6 + 2*g1^7*t^4.383 + 4*g1^2*t^4.681 + (3*t^4.979)/g1^3 + (2*t^5.276)/g1^8 + 3*g1^10*t^5.405 + 5*g1^5*t^5.702 + 2*t^6. + g1^18*t^6.129 + 2*g1^13*t^6.426 + t^6.595/g1^10 + 4*g1^8*t^6.724 + 6*g1^3*t^7.021 + (3*t^7.319)/g1^2 + 2*g1^16*t^7.448 + (2*t^7.617)/g1^7 + 7*g1^11*t^7.745 + (4*t^7.914)/g1^12 + 7*g1^6*t^8.043 + 3*g1^19*t^8.469 - (2*t^8.638)/g1^4 + 7*g1^14*t^8.767 - (2*t^8.936)/g1^9 - t^4.319/(g1^2*y) - t^6.66/(g1*y) - (2*t^6.957)/(g1^6*y) + (3*g1^2*t^7.681)/y + (5*t^7.979)/(g1^3*y) + t^8.276/(g1^8*y) + (2*g1^10*t^8.405)/y + (6*g1^5*t^8.702)/y - (t^4.319*y)/g1^2 - (t^6.66*y)/g1 - (2*t^6.957*y)/g1^6 + 3*g1^2*t^7.681*y + (5*t^7.979*y)/g1^3 + (t^8.276*y)/g1^8 + 2*g1^10*t^8.405*y + 6*g1^5*t^8.702*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 |
---|---|---|---|---|---|---|---|---|
48259 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6629 | 0.8357 | 0.7933 | [M:[0.8819, 1.2205, 0.7795, 0.7795, 0.7795], q:[0.6772, 0.4409], qb:[0.3386, 0.7795], phi:[0.4409]] | 3*t^2.339 + 2*t^2.646 + t^3.047 + 2*t^3.354 + t^3.969 + 2*t^4.37 + 7*t^4.677 + 5*t^4.984 + 2*t^5.291 + 4*t^5.386 + 7*t^5.693 - t^4.323/y - t^4.323*y | detail | |
47036 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}^{2}$ | 0.6351 | 0.7891 | 0.8049 | [M:[0.8956, 1.2239, 0.7761, 0.7761, 1.1044], q:[0.6567, 0.4478], qb:[0.3283, 0.7761], phi:[0.4478]] | 2*t^2.328 + t^2.687 + t^2.955 + 3*t^3.313 + t^3.672 + t^4.03 + 2*t^4.298 + 4*t^4.657 + t^5.015 + 3*t^5.283 + 6*t^5.642 + t^5.91 + t^6. - t^4.343/y - t^4.343*y | detail | |
47248 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ | 0.6514 | 0.8126 | 0.8016 | [M:[0.841, 1.2103, 0.7897, 0.7897, 0.8924], q:[0.7384, 0.4205], qb:[0.3692, 0.7897], phi:[0.4205]] | 2*t^2.369 + 2*t^2.523 + t^2.677 + 2*t^3.477 + t^3.631 + t^3.785 + 2*t^4.584 + 4*t^4.738 + 3*t^4.892 + 4*t^5.046 + 2*t^5.2 + t^5.354 + t^5.692 + 3*t^5.846 + 2*t^6. - t^4.262/y - t^4.262*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
46123 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ | 0.6277 | 0.7724 | 0.8127 | [M:[0.8767, 1.2192, 0.7808], q:[0.6849, 0.4384], qb:[0.3425, 0.7808], phi:[0.4384]] | t^2.342 + 2*t^2.63 + t^3.082 + 2*t^3.37 + 2*t^3.658 + t^3.945 + 2*t^4.397 + 2*t^4.685 + t^4.973 + 2*t^5.26 + 2*t^5.425 + 3*t^5.712 + 2*t^6. - t^4.315/y - t^4.315*y | detail |