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 |
|---|---|---|---|---|---|---|---|---|---|
| 57716 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{3}X_{2}$ | 0.5148 | 0.4823 | 1.0673 | [X:[1.8026, 1.7039], M:[], q:[0.7983, 0.3048], qb:[1.1031, 1.2017], phi:[0.0987]] | [X:[[6], [9]], M:[], q:[[-4], [11]], qb:[[7], [4]], phi:[[-3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}\phi_{1}^{3}q_{2}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$ | ${}$ | -2 | t^3.63 + t^4.22 + t^4.52 - 2*t^6. + t^6.59 + 2*t^6.89 + t^7.18 + t^7.26 + t^7.48 + t^7.78 + t^7.86 + t^8.15 + t^8.37 + t^8.45 + t^6.89/y^2 - t^3.3/y - t^3.59/y - t^7.52/y - t^7.82/y - t^8.11/y - t^8.41/y - t^8.7/y - t^3.3*y - t^3.59*y - t^7.52*y - t^7.82*y - t^8.11*y - t^8.41*y - t^8.7*y + t^6.89*y^2 | g1^24*t^3.63 + g1^18*t^4.22 + g1^15*t^4.52 - 2*t^6. + t^6.59/g1^6 + (2*t^6.89)/g1^9 + t^7.18/g1^12 + g1^48*t^7.26 + t^7.48/g1^15 + t^7.78/g1^18 + g1^42*t^7.86 + g1^39*t^8.15 + t^8.37/g1^24 + g1^36*t^8.45 + t^6.89/(g1^9*y^2) - t^3.3/(g1^3*y) - t^3.59/(g1^6*y) - (g1^15*t^7.52)/y - (g1^12*t^7.82)/y - (g1^9*t^8.11)/y - (g1^6*t^8.41)/y - (g1^3*t^8.7)/y - (t^3.3*y)/g1^3 - (t^3.59*y)/g1^6 - g1^15*t^7.52*y - g1^12*t^7.82*y - g1^9*t^8.11*y - g1^6*t^8.41*y - g1^3*t^8.7*y + (t^6.89*y^2)/g1^9 |
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 |
|---|---|---|---|---|---|---|---|---|
| 60622 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{3}X_{2}$ + ${ }M_{1}\phi_{1}^{3}q_{2}^{3}$ | 0.5335 | 0.5111 | 1.0437 | [X:[1.8165, 1.7247], M:[0.734], q:[0.789, 0.3302], qb:[1.1192, 1.211], phi:[0.0918]] | t^2.2 + t^4.35 + t^4.4 + t^4.62 - 2*t^6. - t^3.28/y - t^3.55/y - t^5.48/y - t^5.75/y - t^3.28*y - t^3.55*y - t^5.48*y - t^5.75*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 47947 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{1}$ | 1.0879 | 1.2082 | 0.9004 | [X:[1.5125], q:[0.6921, 0.372], qb:[1.0641, 0.4092], phi:[0.2437]] | t^2.194 + t^2.344 + t^3.075 + t^3.304 + t^3.806 + t^4.309 + t^4.387 + 2*t^4.538 + t^4.688 + t^5.04 + 2*t^5.269 + t^5.419 + t^5.542 + t^5.648 + t^5.877 - 2*t^6. - t^3.731/y - t^4.462/y - t^5.925/y - t^3.731*y - t^4.462*y - t^5.925*y | detail |