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 |
|---|---|---|---|---|---|---|---|---|---|
| 58829 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{6}$ + ${ }M_{7}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{8}$ | 0.672 | 0.8446 | 0.7956 | [M:[1.1618, 0.8765, 0.8382, 0.7235, 0.7618, 0.8382, 0.7618, 1.2765], q:[0.3618, 0.4765], qb:[0.7618, 0.8], phi:[0.4]] | [M:[[1], [-2], [-1], [2], [1], [-1], [1], [-2]], q:[[1], [-2]], qb:[[1], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{8}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{6}$, ${ }M_{2}^{2}$, ${ }M_{5}\phi_{1}q_{1}^{2}$, ${ }M_{7}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}$ | -3 | 2*t^2.285 + t^2.4 + 2*t^2.515 + t^2.629 + t^3.371 + t^3.829 + t^4.059 + 4*t^4.571 + 3*t^4.685 + 4*t^4.8 + 5*t^4.915 + 4*t^5.029 + t^5.144 + t^5.259 + t^5.656 + 2*t^5.771 + t^5.885 - 3*t^6. + t^6.115 + 2*t^6.344 + 2*t^6.459 + 2*t^6.574 + t^6.688 + t^6.741 + 4*t^6.856 + 4*t^6.971 + 7*t^7.085 + 8*t^7.2 + 8*t^7.315 + 7*t^7.429 + 6*t^7.544 + 2*t^7.659 + t^7.774 + 2*t^7.888 + 2*t^7.941 + 2*t^8.056 + t^8.118 - 5*t^8.285 - 2*t^8.4 - 7*t^8.515 - 2*t^8.629 + 2*t^8.744 + 4*t^8.859 + 4*t^8.974 - t^4.2/y - (2*t^6.485)/y - t^6.6/y - t^6.715/y - t^6.829/y + (2*t^7.571)/y + (3*t^7.685)/y + (5*t^7.8)/y + (6*t^7.915)/y + (2*t^8.029)/y + (2*t^8.144)/y + (2*t^8.656)/y - (2*t^8.771)/y - t^4.2*y - 2*t^6.485*y - t^6.6*y - t^6.715*y - t^6.829*y + 2*t^7.571*y + 3*t^7.685*y + 5*t^7.8*y + 6*t^7.915*y + 2*t^8.029*y + 2*t^8.144*y + 2*t^8.656*y - 2*t^8.771*y | 2*g1*t^2.285 + t^2.4 + (2*t^2.515)/g1 + t^2.629/g1^2 + g1^2*t^3.371 + t^3.829/g1^2 + t^4.059/g1^4 + 4*g1^2*t^4.571 + 3*g1*t^4.685 + 4*t^4.8 + (5*t^4.915)/g1 + (4*t^5.029)/g1^2 + t^5.144/g1^3 + t^5.259/g1^4 + g1^3*t^5.656 + 2*g1^2*t^5.771 + g1*t^5.885 - 3*t^6. + t^6.115/g1 + (2*t^6.344)/g1^3 + (2*t^6.459)/g1^4 + (2*t^6.574)/g1^5 + t^6.688/g1^6 + g1^4*t^6.741 + 4*g1^3*t^6.856 + 4*g1^2*t^6.971 + 7*g1*t^7.085 + 8*t^7.2 + (8*t^7.315)/g1 + (7*t^7.429)/g1^2 + (6*t^7.544)/g1^3 + (2*t^7.659)/g1^4 + t^7.774/g1^5 + (2*t^7.888)/g1^6 + 2*g1^4*t^7.941 + 2*g1^3*t^8.056 + t^8.118/g1^8 - 5*g1*t^8.285 - 2*t^8.4 - (7*t^8.515)/g1 - (2*t^8.629)/g1^2 + (2*t^8.744)/g1^3 + (4*t^8.859)/g1^4 + (4*t^8.974)/g1^5 - t^4.2/y - (2*g1*t^6.485)/y - t^6.6/y - t^6.715/(g1*y) - t^6.829/(g1^2*y) + (2*g1^2*t^7.571)/y + (3*g1*t^7.685)/y + (5*t^7.8)/y + (6*t^7.915)/(g1*y) + (2*t^8.029)/(g1^2*y) + (2*t^8.144)/(g1^3*y) + (2*g1^3*t^8.656)/y - (2*g1^2*t^8.771)/y - t^4.2*y - 2*g1*t^6.485*y - t^6.6*y - (t^6.715*y)/g1 - (t^6.829*y)/g1^2 + 2*g1^2*t^7.571*y + 3*g1*t^7.685*y + 5*t^7.8*y + (6*t^7.915*y)/g1 + (2*t^8.029*y)/g1^2 + (2*t^8.144*y)/g1^3 + 2*g1^3*t^8.656*y - 2*g1^2*t^8.771*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 |
|---|---|---|---|---|---|---|---|---|---|
| 56950 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{6}$ + ${ }M_{7}q_{2}\tilde{q}_{1}$ | 0.6921 | 0.8823 | 0.7845 | [M:[1.1575, 0.885, 0.8425, 0.715, 0.7575, 0.8425, 0.7575], q:[0.3575, 0.485], qb:[0.7575, 0.8], phi:[0.4]] | t^2.145 + 2*t^2.273 + t^2.4 + 2*t^2.527 + t^2.655 + t^3.345 + t^4.11 + t^4.29 + 2*t^4.418 + 5*t^4.545 + 5*t^4.673 + 5*t^4.8 + 5*t^4.927 + 4*t^5.055 + t^5.182 + t^5.31 + t^5.49 + t^5.618 + 2*t^5.745 + t^5.873 - 3*t^6. - t^4.2/y - t^4.2*y | detail |