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 |
|---|---|---|---|---|---|---|---|---|---|
| 56605 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{6}M_{7}$ | 0.6526 | 0.8114 | 0.8042 | [M:[1.1707, 0.8585, 0.8293, 0.7415, 0.8585, 0.7707, 1.2293], q:[0.3707, 0.4585], qb:[0.7707, 0.8], phi:[0.4]] | [M:[[1], [-2], [-1], [2], [-2], [1], [-1]], q:[[1], [-2]], qb:[[1], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{2}$, ${ }M_{5}$, ${ }M_{1}$, ${ }M_{7}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}$ | -3 | t^2.224 + t^2.4 + t^2.488 + 2*t^2.576 + t^3.512 + 2*t^3.688 + t^3.951 + t^4.449 + 2*t^4.624 + 2*t^4.712 + 2*t^4.8 + 2*t^4.888 + 3*t^4.976 + t^5.063 + 3*t^5.151 + t^5.824 + 2*t^5.912 - 3*t^6. + 3*t^6.088 + 2*t^6.176 + 2*t^6.263 + t^6.351 + t^6.439 + 2*t^6.527 + t^6.673 + 2*t^6.849 + 2*t^7.024 + 2*t^7.112 + 3*t^7.2 + 2*t^7.288 + 7*t^7.376 + 3*t^7.463 + 3*t^7.551 + 3*t^7.639 + 4*t^7.727 + t^7.902 + t^8.049 - 3*t^8.224 + t^8.312 - t^8.488 - 3*t^8.576 + 5*t^8.663 + t^8.751 + 4*t^8.839 + t^8.898 + 3*t^8.927 - t^4.2/y - t^6.424/y - t^6.6/y - (2*t^6.776)/y + (3*t^7.624)/y + t^7.712/y + (3*t^7.8)/y + t^7.888/y + (3*t^7.976)/y + (2*t^8.063)/y + t^8.151/y - t^8.649/y + t^8.737/y - t^8.824/y + (3*t^8.912)/y - t^4.2*y - t^6.424*y - t^6.6*y - 2*t^6.776*y + 3*t^7.624*y + t^7.712*y + 3*t^7.8*y + t^7.888*y + 3*t^7.976*y + 2*t^8.063*y + t^8.151*y - t^8.649*y + t^8.737*y - t^8.824*y + 3*t^8.912*y | g1^2*t^2.224 + t^2.4 + t^2.488/g1 + (2*t^2.576)/g1^2 + g1*t^3.512 + (2*t^3.688)/g1 + t^3.951/g1^4 + g1^4*t^4.449 + 2*g1^2*t^4.624 + 2*g1*t^4.712 + 2*t^4.8 + (2*t^4.888)/g1 + (3*t^4.976)/g1^2 + t^5.063/g1^3 + (3*t^5.151)/g1^4 + g1^2*t^5.824 + 2*g1*t^5.912 - 3*t^6. + (3*t^6.088)/g1 + (2*t^6.176)/g1^2 + (2*t^6.263)/g1^3 + t^6.351/g1^4 + t^6.439/g1^5 + (2*t^6.527)/g1^6 + g1^6*t^6.673 + 2*g1^4*t^6.849 + 2*g1^2*t^7.024 + 2*g1*t^7.112 + 3*t^7.2 + (2*t^7.288)/g1 + (7*t^7.376)/g1^2 + (3*t^7.463)/g1^3 + (3*t^7.551)/g1^4 + (3*t^7.639)/g1^5 + (4*t^7.727)/g1^6 + t^7.902/g1^8 + g1^4*t^8.049 - 3*g1^2*t^8.224 + g1*t^8.312 - t^8.488/g1 - (3*t^8.576)/g1^2 + (5*t^8.663)/g1^3 + t^8.751/g1^4 + (4*t^8.839)/g1^5 + g1^8*t^8.898 + (3*t^8.927)/g1^6 - t^4.2/y - (g1^2*t^6.424)/y - t^6.6/y - (2*t^6.776)/(g1^2*y) + (3*g1^2*t^7.624)/y + (g1*t^7.712)/y + (3*t^7.8)/y + t^7.888/(g1*y) + (3*t^7.976)/(g1^2*y) + (2*t^8.063)/(g1^3*y) + t^8.151/(g1^4*y) - (g1^4*t^8.649)/y + (g1^3*t^8.737)/y - (g1^2*t^8.824)/y + (3*g1*t^8.912)/y - t^4.2*y - g1^2*t^6.424*y - t^6.6*y - (2*t^6.776*y)/g1^2 + 3*g1^2*t^7.624*y + g1*t^7.712*y + 3*t^7.8*y + (t^7.888*y)/g1 + (3*t^7.976*y)/g1^2 + (2*t^8.063*y)/g1^3 + (t^8.151*y)/g1^4 - g1^4*t^8.649*y + g1^3*t^8.737*y - g1^2*t^8.824*y + 3*g1*t^8.912*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 |
|---|---|---|---|---|---|---|---|---|---|
| 54780 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ | 0.6708 | 0.8437 | 0.795 | [M:[1.1673, 0.8655, 0.8327, 0.7345, 0.8655, 0.7673], q:[0.3673, 0.4655], qb:[0.7673, 0.8], phi:[0.4]] | t^2.204 + t^2.302 + t^2.4 + t^2.498 + 2*t^2.596 + t^3.502 + t^3.698 + t^3.993 + t^4.407 + t^4.505 + 3*t^4.604 + 3*t^4.702 + 3*t^4.8 + 4*t^4.898 + 3*t^4.996 + t^5.095 + 3*t^5.193 + 2*t^5.804 + t^5.902 - 2*t^6. - t^4.2/y - t^4.2*y | detail |