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 |
|---|---|---|---|---|---|---|---|---|---|
| 6409 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{3}M_{8}$ + ${ }M_{6}M_{8}$ + ${ }M_{6}M_{9}$ | 0.6526 | 0.8114 | 0.8042 | [M:[0.8585, 0.7415, 0.7707, 0.8293, 1.1707, 0.7707, 0.8585, 1.2293, 1.2293], q:[0.7707, 0.3707], qb:[0.4585, 0.8], phi:[0.4]] | [M:[[2], [-2], [-1], [1], [-1], [-1], [2], [1], [1]], q:[[-1], [-1]], qb:[[2], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{1}$, ${ }M_{7}$, ${ }M_{5}$, ${ }M_{8}$, ${ }M_{9}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}M_{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{7}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}M_{8}$, ${ }M_{2}M_{9}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | ${}$ | -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 | t^2.224/g1^2 + t^2.4 + g1*t^2.488 + 2*g1^2*t^2.576 + t^3.512/g1 + 2*g1*t^3.688 + g1^4*t^3.951 + t^4.449/g1^4 + (2*t^4.624)/g1^2 + (2*t^4.712)/g1 + 2*t^4.8 + 2*g1*t^4.888 + 3*g1^2*t^4.976 + g1^3*t^5.063 + 3*g1^4*t^5.151 + t^5.824/g1^2 + (2*t^5.912)/g1 - 3*t^6. + 3*g1*t^6.088 + 2*g1^2*t^6.176 + 2*g1^3*t^6.263 + g1^4*t^6.351 + g1^5*t^6.439 + 2*g1^6*t^6.527 + t^6.673/g1^6 + (2*t^6.849)/g1^4 + (2*t^7.024)/g1^2 + (2*t^7.112)/g1 + 3*t^7.2 + 2*g1*t^7.288 + 7*g1^2*t^7.376 + 3*g1^3*t^7.463 + 3*g1^4*t^7.551 + 3*g1^5*t^7.639 + 4*g1^6*t^7.727 + g1^8*t^7.902 + t^8.049/g1^4 - (3*t^8.224)/g1^2 + t^8.312/g1 - g1*t^8.488 - 3*g1^2*t^8.576 + 5*g1^3*t^8.663 + g1^4*t^8.751 + 4*g1^5*t^8.839 + t^8.898/g1^8 + 3*g1^6*t^8.927 - t^4.2/y - t^6.424/(g1^2*y) - t^6.6/y - (2*g1^2*t^6.776)/y + (3*t^7.624)/(g1^2*y) + t^7.712/(g1*y) + (3*t^7.8)/y + (g1*t^7.888)/y + (3*g1^2*t^7.976)/y + (2*g1^3*t^8.063)/y + (g1^4*t^8.151)/y - t^8.649/(g1^4*y) + t^8.737/(g1^3*y) - t^8.824/(g1^2*y) + (3*t^8.912)/(g1*y) - t^4.2*y - (t^6.424*y)/g1^2 - t^6.6*y - 2*g1^2*t^6.776*y + (3*t^7.624*y)/g1^2 + (t^7.712*y)/g1 + 3*t^7.8*y + g1*t^7.888*y + 3*g1^2*t^7.976*y + 2*g1^3*t^8.063*y + g1^4*t^8.151*y - (t^8.649*y)/g1^4 + (t^8.737*y)/g1^3 - (t^8.824*y)/g1^2 + (3*t^8.912*y)/g1 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 4801 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{3}M_{8}$ + ${ }M_{6}M_{8}$ | 0.6708 | 0.8437 | 0.795 | [M:[0.8655, 0.7345, 0.7673, 0.8327, 1.1673, 0.7673, 0.8655, 1.2327], q:[0.7673, 0.3673], qb:[0.4655, 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 |