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 |
|---|---|---|---|---|---|---|---|---|---|
| 58066 | SU3adj1nf2 | ${}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}q_{2}\tilde{q}_{2}$ | 1.1499 | 1.2998 | 0.8847 | [X:[1.5338], M:[0.7004, 0.6993], q:[0.8682, 0.4009], qb:[0.8987, 0.4336], phi:[0.2331]] | [X:[[0, 2]], M:[[-1, -4], [0, -3]], q:[[-1, 1], [0, 4]], qb:[[1, 0], [0, 1]], phi:[[0, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{6}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | -1 | 3*t^2.1 + t^2.5 + t^3.2 + t^3.91 + 6*t^4.2 + 4*t^4.6 + t^5.01 + 4*t^5.3 + 3*t^5.71 - t^6. + t^6.01 + 4*t^6.29 + 6*t^6.3 + 2*t^6.41 + 7*t^6.7 + t^6.71 + 3*t^7.1 + 2*t^7.11 + 6*t^7.4 + t^7.51 + 4*t^7.8 + 5*t^7.81 - t^8.09 - 3*t^8.1 + t^8.11 + 3*t^8.21 + 9*t^8.39 + 6*t^8.4 - t^8.5 + 3*t^8.51 - t^8.79 + 6*t^8.8 + t^8.81 + 4*t^8.91 + t^8.1/y^2 - (3*t^8.8)/y^2 - t^3.7/y - t^4.4/y - (3*t^5.8)/y - t^6.2/y - (3*t^6.5)/y - t^6.9/y + (3*t^7.2)/y + (2*t^7.6)/y - (6*t^7.9)/y + (2*t^8.3)/y - (3*t^8.59)/y - (3*t^8.6)/y - t^3.7*y - t^4.4*y - 3*t^5.8*y - t^6.2*y - 3*t^6.5*y - t^6.9*y + 3*t^7.2*y + 2*t^7.6*y - 6*t^7.9*y + 2*t^8.3*y - 3*t^8.59*y - 3*t^8.6*y + t^8.1*y^2 - 3*t^8.8*y^2 | t^2.1/(g1*g2^4) + (2*t^2.1)/g2^3 + g2^5*t^2.5 + g2^4*t^3.2 + (g2^2*t^3.91)/g1 + t^4.2/(g1^2*g2^8) + (2*t^4.2)/(g1*g2^7) + (3*t^4.2)/g2^6 + (g2*t^4.6)/g1 + 3*g2^2*t^4.6 + g2^10*t^5.01 + t^5.3/g1 + 3*g2*t^5.3 + (g2^8*t^5.71)/g1 + 2*g2^9*t^5.71 - 2*t^6. + t^6./(g1*g2) + t^6.01/(g1^2*g2^2) + (4*t^6.29)/g2^9 + t^6.3/(g1^3*g2^12) + (2*t^6.3)/(g1^2*g2^11) + (3*t^6.3)/(g1*g2^10) + (g2^7*t^6.41)/g1 + g2^8*t^6.41 + (3*t^6.7)/(g1*g2^2) + (4*t^6.7)/g2 + t^6.71/(g1^2*g2^3) + 3*g2^7*t^7.1 + (2*g2^6*t^7.11)/g1 + t^7.4/(g1^2*g2^4) + (2*t^7.4)/(g1*g2^3) + (4*t^7.4)/g2^2 - (g1*t^7.4)/g2 + g2^15*t^7.51 + 4*g2^6*t^7.8 + (2*g2^4*t^7.81)/g1^2 + (3*g2^5*t^7.81)/g1 - (g1*t^8.09)/g2^2 + t^8.1/(g1^2*g2^5) - t^8.1/(g1*g2^4) - (3*t^8.1)/g2^3 + t^8.11/(g1^3*g2^6) + (g2^13*t^8.21)/g1 + 2*g2^14*t^8.21 + (4*t^8.39)/(g1*g2^13) + (5*t^8.39)/g2^12 + t^8.4/(g1^4*g2^16) + (2*t^8.4)/(g1^3*g2^15) + (3*t^8.4)/(g1^2*g2^14) - g2^5*t^8.5 + (g2^3*t^8.51)/g1^2 + (2*g2^4*t^8.51)/g1 - (g1*t^8.79)/g2^3 + (3*t^8.8)/(g1^2*g2^6) + (2*t^8.8)/(g1*g2^5) + t^8.8/g2^4 + t^8.81/(g1^3*g2^7) + (2*g2^12*t^8.91)/g1 + 2*g2^13*t^8.91 + t^8.1/(g2^3*y^2) - t^8.8/(g1*g2^5*y^2) - (2*t^8.8)/(g2^4*y^2) - t^3.7/(g2*y) - t^4.4/(g2^2*y) - t^5.8/(g1*g2^5*y) - (2*t^5.8)/(g2^4*y) - (g2^4*t^6.2)/y - t^6.5/(g1*g2^6*y) - (2*t^6.5)/(g2^5*y) - (g2^3*t^6.9)/y + (2*t^7.2)/(g1*g2^7*y) + t^7.2/(g2^6*y) + (2*g2^2*t^7.6)/y - t^7.9/(g1^2*g2^9*y) - (2*t^7.9)/(g1*g2^8*y) - (3*t^7.9)/(g2^7*y) + (g2*t^8.3)/y + (g1*g2^2*t^8.3)/y - (3*t^8.59)/(g2^8*y) - t^8.6/(g1^2*g2^10*y) - (2*t^8.6)/(g1*g2^9*y) - (t^3.7*y)/g2 - (t^4.4*y)/g2^2 - (t^5.8*y)/(g1*g2^5) - (2*t^5.8*y)/g2^4 - g2^4*t^6.2*y - (t^6.5*y)/(g1*g2^6) - (2*t^6.5*y)/g2^5 - g2^3*t^6.9*y + (2*t^7.2*y)/(g1*g2^7) + (t^7.2*y)/g2^6 + 2*g2^2*t^7.6*y - (t^7.9*y)/(g1^2*g2^9) - (2*t^7.9*y)/(g1*g2^8) - (3*t^7.9*y)/g2^7 + g2*t^8.3*y + g1*g2^2*t^8.3*y - (3*t^8.59*y)/g2^8 - (t^8.6*y)/(g1^2*g2^10) - (2*t^8.6*y)/(g1*g2^9) + (t^8.1*y^2)/g2^3 - (t^8.8*y^2)/(g1*g2^5) - (2*t^8.8*y^2)/g2^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 57324 | SU3adj1nf2 | ${}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ | 1.1294 | 1.2609 | 0.8957 | [X:[1.5322], M:[0.7029], q:[0.8668, 0.3978], qb:[0.8993, 0.4328], phi:[0.2339]] | t^2.105 + t^2.109 + t^2.492 + t^3.193 + t^3.895 + t^3.899 + t^4.21 + t^4.214 + t^4.217 + 2*t^4.597 + t^4.6 + t^4.983 + 2*t^5.298 + t^5.302 + 2*t^5.685 + t^5.689 - t^6. - t^3.702/y - t^4.403/y - t^5.807/y - t^5.81/y - t^3.702*y - t^4.403*y - t^5.807*y - t^5.81*y | detail |