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 |
|---|---|---|---|---|---|---|---|---|---|
| 58473 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}X_{2}$ | 1.1263 | 1.3138 | 0.8573 | [X:[1.3243, 1.3514], M:[0.7028], q:[0.3379, 0.9864], qb:[0.3379, 0.3107], phi:[0.3379]] | [X:[[-2], [4]], M:[[8]], q:[[1], [-3]], qb:[[1], [-5]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }X_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{4}q_{1}\tilde{q}_{2}$, ${ 2}\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}X_{1}$ | 4 | t^2.03 + t^2.11 + t^2.96 + 2*t^3.04 + t^3.89 + 4*t^3.97 + 2*t^4.05 + t^4.14 + t^4.22 + 2*t^4.91 + 2*t^4.99 + 2*t^5.07 + 2*t^5.15 + t^5.84 + 2*t^5.92 + 4*t^6. + 8*t^6.08 + 2*t^6.16 + t^6.24 + t^6.33 + t^6.85 + 3*t^6.93 + 9*t^7.01 + 4*t^7.09 + 2*t^7.18 + 2*t^7.26 + t^7.78 + 4*t^7.86 + 11*t^7.95 + 7*t^8.03 + 6*t^8.11 + 8*t^8.19 + 2*t^8.27 + t^8.35 + t^8.43 + 2*t^8.8 + 7*t^8.88 + 2*t^8.96 - t^4.01/y - t^5.03/y - t^6.04/y - t^6.12/y - (2*t^7.05)/y - t^7.99/y + t^8.15/y - t^8.23/y + t^8.92/y - t^4.01*y - t^5.03*y - t^6.04*y - t^6.12*y - 2*t^7.05*y - t^7.99*y + t^8.15*y - t^8.23*y + t^8.92*y | g1^2*t^2.03 + g1^8*t^2.11 + t^2.96/g1^3 + 2*g1^3*t^3.04 + t^3.89/g1^8 + (4*t^3.97)/g1^2 + 2*g1^4*t^4.05 + g1^10*t^4.14 + g1^16*t^4.22 + (2*t^4.91)/g1^7 + (2*t^4.99)/g1 + 2*g1^5*t^5.07 + 2*g1^11*t^5.15 + t^5.84/g1^12 + (2*t^5.92)/g1^6 + 4*t^6. + 8*g1^6*t^6.08 + 2*g1^12*t^6.16 + g1^18*t^6.24 + g1^24*t^6.33 + t^6.85/g1^11 + (3*t^6.93)/g1^5 + 9*g1*t^7.01 + 4*g1^7*t^7.09 + 2*g1^13*t^7.18 + 2*g1^19*t^7.26 + t^7.78/g1^16 + (4*t^7.86)/g1^10 + (11*t^7.95)/g1^4 + 7*g1^2*t^8.03 + 6*g1^8*t^8.11 + 8*g1^14*t^8.19 + 2*g1^20*t^8.27 + g1^26*t^8.35 + g1^32*t^8.43 + (2*t^8.8)/g1^15 + (7*t^8.88)/g1^9 + (2*t^8.96)/g1^3 - (g1*t^4.01)/y - (g1^2*t^5.03)/y - (g1^3*t^6.04)/y - (g1^9*t^6.12)/y - (2*g1^4*t^7.05)/y - t^7.99/(g1*y) + (g1^11*t^8.15)/y - (g1^17*t^8.23)/y + t^8.92/(g1^6*y) - g1*t^4.01*y - g1^2*t^5.03*y - g1^3*t^6.04*y - g1^9*t^6.12*y - 2*g1^4*t^7.05*y - (t^7.99*y)/g1 + g1^11*t^8.15*y - g1^17*t^8.23*y + (t^8.92*y)/g1^6 |
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 |
|---|---|---|---|---|---|---|---|---|
| 61199 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}X_{2}$ + ${ }M_{2}\phi_{1}^{3}$ | 1.1279 | 1.3166 | 0.8566 | [X:[1.3198, 1.3605], M:[0.721, 0.9796], q:[0.3401, 0.9796], qb:[0.3401, 0.2994], phi:[0.3401]] | t^2.04 + t^2.16 + 2*t^2.94 + t^3.06 + t^3.84 + 4*t^3.96 + 2*t^4.08 + t^4.2 + t^4.33 + 2*t^4.86 + 3*t^4.98 + 2*t^5.1 + t^5.22 + t^5.76 + 4*t^5.88 + 4*t^6. - t^4.02/y - t^5.04/y - t^4.02*y - t^5.04*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57380 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ | 1.4443 | 1.6269 | 0.8878 | [X:[1.3565], M:[0.9391], q:[0.5652, 0.5479], qb:[0.4435, 0.513], phi:[0.3217]] | t^2.817 + t^2.896 + t^2.974 + t^3.026 + t^3.235 + t^3.939 + t^3.991 + t^4.07 + t^4.148 + t^4.2 + t^4.904 + t^4.956 + t^5.113 + 2*t^5.165 + t^5.374 + t^5.634 + t^5.713 + t^5.791 + t^5.843 + t^5.87 + t^5.922 + t^5.948 - 2*t^6. - t^3.965/y - t^4.93/y - t^3.965*y - t^4.93*y | detail |