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 |
|---|---|---|---|---|---|---|---|---|---|
| 56743 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ + ${ }M_{4}M_{6}$ + ${ }M_{7}\phi_{1}q_{1}q_{2}$ | 0.6518 | 0.8129 | 0.8018 | [M:[1.1554, 0.733, 0.8446, 0.8074, 0.8446, 1.1926, 0.7702], q:[0.4037, 0.4409], qb:[0.8633, 0.7516], phi:[0.3851]] | [M:[[12], [18], [-12], [-2], [-12], [2], [8]], q:[[-1], [-11]], qb:[[-17], [13]], phi:[[4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}^{2}$ | ${}M_{2}\phi_{1}q_{2}^{2}$ | -2 | t^2.199 + 2*t^2.311 + 2*t^2.534 + 2*t^3.578 + t^3.801 + t^3.913 + t^4.398 + 2*t^4.51 + 3*t^4.621 + 2*t^4.733 + 5*t^4.845 + 3*t^5.068 + t^5.777 + 2*t^5.888 - 2*t^6. + 5*t^6.112 + t^6.223 + 2*t^6.335 + 2*t^6.446 + t^6.597 + 2*t^6.709 + 3*t^6.82 + 5*t^6.932 + 3*t^7.044 + 8*t^7.155 - t^7.267 + 6*t^7.379 + 4*t^7.602 + t^7.713 + t^7.825 + t^7.976 - 3*t^8.311 + 4*t^8.422 - 5*t^8.534 + 7*t^8.646 + 2*t^8.757 + t^8.796 + 3*t^8.869 + 2*t^8.908 + 3*t^8.98 - t^4.155/y - t^6.354/y - (2*t^6.466)/y - t^6.689/y + (2*t^7.51)/y + (2*t^7.621)/y + (2*t^7.733)/y + (6*t^7.845)/y + t^7.956/y + t^8.068/y - t^8.554/y - (2*t^8.665)/y - t^8.777/y + (3*t^8.888)/y - t^4.155*y - t^6.354*y - 2*t^6.466*y - t^6.689*y + 2*t^7.51*y + 2*t^7.621*y + 2*t^7.733*y + 6*t^7.845*y + t^7.956*y + t^8.068*y - t^8.554*y - 2*t^8.665*y - t^8.777*y + 3*t^8.888*y | g1^18*t^2.199 + 2*g1^8*t^2.311 + (2*t^2.534)/g1^12 + 2*g1^2*t^3.578 + t^3.801/g1^18 + t^3.913/g1^28 + g1^36*t^4.398 + 2*g1^26*t^4.51 + 3*g1^16*t^4.621 + 2*g1^6*t^4.733 + (5*t^4.845)/g1^4 + (3*t^5.068)/g1^24 + g1^20*t^5.777 + 2*g1^10*t^5.888 - 2*t^6. + (5*t^6.112)/g1^10 + t^6.223/g1^20 + (2*t^6.335)/g1^30 + (2*t^6.446)/g1^40 + g1^54*t^6.597 + 2*g1^44*t^6.709 + 3*g1^34*t^6.82 + 5*g1^24*t^6.932 + 3*g1^14*t^7.044 + 8*g1^4*t^7.155 - t^7.267/g1^6 + (6*t^7.379)/g1^16 + (4*t^7.602)/g1^36 + t^7.713/g1^46 + t^7.825/g1^56 + g1^38*t^7.976 - 3*g1^8*t^8.311 + (4*t^8.422)/g1^2 - (5*t^8.534)/g1^12 + (7*t^8.646)/g1^22 + (2*t^8.757)/g1^32 + g1^72*t^8.796 + (3*t^8.869)/g1^42 + 2*g1^62*t^8.908 + (3*t^8.98)/g1^52 - (g1^4*t^4.155)/y - (g1^22*t^6.354)/y - (2*g1^12*t^6.466)/y - t^6.689/(g1^8*y) + (2*g1^26*t^7.51)/y + (2*g1^16*t^7.621)/y + (2*g1^6*t^7.733)/y + (6*t^7.845)/(g1^4*y) + t^7.956/(g1^14*y) + t^8.068/(g1^24*y) - (g1^40*t^8.554)/y - (2*g1^30*t^8.665)/y - (g1^20*t^8.777)/y + (3*g1^10*t^8.888)/y - g1^4*t^4.155*y - g1^22*t^6.354*y - 2*g1^12*t^6.466*y - (t^6.689*y)/g1^8 + 2*g1^26*t^7.51*y + 2*g1^16*t^7.621*y + 2*g1^6*t^7.733*y + (6*t^7.845*y)/g1^4 + (t^7.956*y)/g1^14 + (t^8.068*y)/g1^24 - g1^40*t^8.554*y - 2*g1^30*t^8.665*y - g1^20*t^8.777*y + 3*g1^10*t^8.888*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 |
|---|
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 |
|---|
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 55092 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ + ${ }M_{4}M_{6}$ | 0.6338 | 0.781 | 0.8115 | [M:[1.1617, 0.7426, 0.8383, 0.8064, 0.8383, 1.1936], q:[0.4032, 0.4351], qb:[0.8542, 0.7585], phi:[0.3872]] | t^2.228 + t^2.323 + 2*t^2.515 + 2*t^3.581 + t^3.677 + t^3.772 + t^3.868 + t^4.456 + t^4.551 + t^4.647 + 2*t^4.743 + 3*t^4.838 + 3*t^5.03 + t^5.809 + t^5.904 - t^6. - t^4.162/y - t^4.162*y | detail |