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 |
|---|---|---|---|---|---|---|---|---|---|
| 2058 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ | 0.7155 | 0.8872 | 0.8065 | [M:[1.0, 0.9105, 1.0895, 0.821, 0.9105, 0.9105], q:[0.4105, 0.5895], qb:[0.5, 0.5895], phi:[0.4776]] | [M:[[0], [-4], [4], [-8], [-4], [-4]], q:[[-4], [4]], qb:[[0], [4]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$ | ${}q_{1}^{2}\tilde{q}_{2}^{2}$ | -3 | t^2.463 + 3*t^2.732 + t^2.866 + 2*t^3. + t^3.896 + t^4.164 + 3*t^4.433 + 2*t^4.701 + t^4.926 + 3*t^4.97 + 3*t^5.195 + t^5.329 + 6*t^5.463 + 3*t^5.597 + 4*t^5.732 + 2*t^5.866 - 3*t^6. - 4*t^6.268 + t^6.359 - 2*t^6.537 + 4*t^6.628 + t^6.762 + 6*t^6.896 + 8*t^7.164 + 2*t^7.299 + t^7.389 + 7*t^7.433 - t^7.567 + 3*t^7.658 + 5*t^7.701 + 2*t^7.792 + t^7.836 + 6*t^7.926 + t^7.97 + 4*t^8.061 - 3*t^8.104 + 8*t^8.195 - 2*t^8.238 + 9*t^8.329 + 2*t^8.463 + 7*t^8.597 - 12*t^8.732 + t^8.822 + 3*t^8.866 - t^4.433/y - t^6.896/y - (2*t^7.164)/y - t^7.299/y + t^7.567/y + (2*t^7.701)/y + t^7.97/y + (3*t^8.195)/y + t^8.329/y + (5*t^8.463)/y + (3*t^8.597)/y + (6*t^8.732)/y + (2*t^8.866)/y - t^4.433*y - t^6.896*y - 2*t^7.164*y - t^7.299*y + t^7.567*y + 2*t^7.701*y + t^7.97*y + 3*t^8.195*y + t^8.329*y + 5*t^8.463*y + 3*t^8.597*y + 6*t^8.732*y + 2*t^8.866*y | t^2.463/g1^8 + (3*t^2.732)/g1^4 + t^2.866/g1^2 + 2*t^3. + t^3.896/g1^9 + t^4.164/g1^5 + (3*t^4.433)/g1 + 2*g1^3*t^4.701 + t^4.926/g1^16 + 3*g1^7*t^4.97 + (3*t^5.195)/g1^12 + t^5.329/g1^10 + (6*t^5.463)/g1^8 + (3*t^5.597)/g1^6 + (4*t^5.732)/g1^4 + (2*t^5.866)/g1^2 - 3*t^6. - 4*g1^4*t^6.268 + t^6.359/g1^17 - 2*g1^8*t^6.537 + (4*t^6.628)/g1^13 + t^6.762/g1^11 + (6*t^6.896)/g1^9 + (8*t^7.164)/g1^5 + (2*t^7.299)/g1^3 + t^7.389/g1^24 + (7*t^7.433)/g1 - g1*t^7.567 + (3*t^7.658)/g1^20 + 5*g1^3*t^7.701 + (2*t^7.792)/g1^18 + g1^5*t^7.836 + (6*t^7.926)/g1^16 + g1^7*t^7.97 + (4*t^8.061)/g1^14 - 3*g1^9*t^8.104 + (8*t^8.195)/g1^12 - 2*g1^11*t^8.238 + (9*t^8.329)/g1^10 + (2*t^8.463)/g1^8 + (7*t^8.597)/g1^6 - (12*t^8.732)/g1^4 + t^8.822/g1^25 + (3*t^8.866)/g1^2 - t^4.433/(g1*y) - t^6.896/(g1^9*y) - (2*t^7.164)/(g1^5*y) - t^7.299/(g1^3*y) + (g1*t^7.567)/y + (2*g1^3*t^7.701)/y + (g1^7*t^7.97)/y + (3*t^8.195)/(g1^12*y) + t^8.329/(g1^10*y) + (5*t^8.463)/(g1^8*y) + (3*t^8.597)/(g1^6*y) + (6*t^8.732)/(g1^4*y) + (2*t^8.866)/(g1^2*y) - (t^4.433*y)/g1 - (t^6.896*y)/g1^9 - (2*t^7.164*y)/g1^5 - (t^7.299*y)/g1^3 + g1*t^7.567*y + 2*g1^3*t^7.701*y + g1^7*t^7.97*y + (3*t^8.195*y)/g1^12 + (t^8.329*y)/g1^10 + (5*t^8.463*y)/g1^8 + (3*t^8.597*y)/g1^6 + (6*t^8.732*y)/g1^4 + (2*t^8.866*y)/g1^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 889 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ | 0.708 | 0.8725 | 0.8115 | [M:[1.0, 0.9246, 1.0754, 0.8491, 0.9246], q:[0.4246, 0.5754], qb:[0.5, 0.5754], phi:[0.4811]] | t^2.547 + 2*t^2.774 + t^2.887 + 2*t^3. + t^3.226 + t^3.991 + t^4.217 + 3*t^4.443 + 2*t^4.67 + 3*t^4.896 + t^5.095 + 2*t^5.321 + t^5.434 + 3*t^5.547 + 2*t^5.66 + 3*t^5.774 + 2*t^5.887 - t^6. - t^4.443/y - t^4.443*y | detail |