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 |
|---|---|---|---|---|---|---|---|---|---|
| 59064 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.3912 | 1.5609 | 0.8913 | [X:[1.4286], M:[0.9861, 0.7282], q:[0.5736, 0.5457], qb:[0.4404, 0.7261], phi:[0.2857]] | [X:[[0, 0]], M:[[1, 1], [-1, -1]], q:[[-1, -2], [1, 0]], qb:[[0, 1], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }\phi_{1}^{3}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{6}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$ | ${}$ | -4 | t^2.18 + t^2.57 + 2*t^2.96 + t^3.82 + 2*t^3.9 + t^4.29 + t^4.37 + 2*t^4.67 + 3*t^4.76 + 2*t^5.14 + 3*t^5.53 + t^5.61 + t^5.68 + t^5.85 + 2*t^5.92 + t^5.94 - 4*t^6. + t^6.08 + t^6.39 + 3*t^6.47 + 3*t^6.53 + t^6.55 + t^6.71 + t^6.77 + t^6.79 + 2*t^6.86 + 2*t^6.94 - t^7.18 + 4*t^7.24 + 4*t^7.33 + 2*t^7.39 + t^7.48 + t^7.57 + 4*t^7.63 + t^7.65 + 6*t^7.71 + t^7.73 - 2*t^7.78 + 3*t^7.8 - t^7.86 - t^7.95 - 2*t^8.04 + 4*t^8.1 - t^8.18 + 2*t^8.25 + t^8.27 + t^8.42 + 6*t^8.49 + t^8.51 + 4*t^8.57 - t^8.64 + 6*t^8.66 + t^8.74 + 2*t^8.87 - t^8.89 - 7*t^8.96 - t^8.98 + t^8.57/y^2 - t^3.86/y - t^4.71/y - t^6.04/y - t^6.43/y - (2*t^6.82)/y - t^6.9/y - t^7.29/y - (2*t^7.67)/y + (2*t^8.14)/y - t^8.23/y + t^8.53/y - (3*t^8.61)/y + t^8.92/y - t^3.86*y - t^4.71*y - t^6.04*y - t^6.43*y - 2*t^6.82*y - t^6.9*y - t^7.29*y - 2*t^7.67*y + 2*t^8.14*y - t^8.23*y + t^8.53*y - 3*t^8.61*y + t^8.92*y + t^8.57*y^2 | t^2.18/(g1*g2) + t^2.57 + 2*g1*g2*t^2.96 + g1*g2*t^3.82 + (2*t^3.9)/(g1*g2) + t^4.29 + t^4.37/(g1^2*g2^2) + 2*g1*g2*t^4.67 + (3*t^4.76)/(g1*g2) + 2*t^5.14 + 3*g1*g2*t^5.53 + t^5.61/(g1*g2) + g2^3*t^5.68 + (g1*t^5.85)/g2^2 + 2*g1^2*g2^2*t^5.92 + t^5.94/(g1*g2^4) - 4*t^6. + t^6.08/(g1^2*g2^2) + g1*g2*t^6.39 + (3*t^6.47)/(g1*g2) + 3*g2^3*t^6.53 + t^6.55/(g1^3*g2^3) + (g1*t^6.71)/g2^2 + g1^2*g2^2*t^6.77 + t^6.79/(g1*g2^4) + 2*t^6.86 + (2*t^6.94)/(g1^2*g2^2) - t^7.18/g2^3 + 4*g1*g2*t^7.24 + (4*t^7.33)/(g1*g2) + 2*g2^3*t^7.39 + g1^3*t^7.48 + (g1*t^7.57)/g2^2 + 4*g1^2*g2^2*t^7.63 + t^7.65/(g1*g2^4) + 6*t^7.71 + t^7.73/(g1^3*g2^6) - 2*g1*g2^4*t^7.78 + (3*t^7.8)/(g1^2*g2^2) - (g2^2*t^7.86)/g1 - (g1^2*t^7.95)/g2 - (2*t^8.04)/g2^3 + 4*g1*g2*t^8.1 - t^8.18/(g1*g2) + 2*g2^3*t^8.25 + t^8.27/(g1^3*g2^3) + (g1*t^8.42)/g2^2 + 6*g1^2*g2^2*t^8.49 + t^8.51/(g1*g2^4) + 4*t^8.57 - g1*g2^4*t^8.64 + (6*t^8.66)/(g1^2*g2^2) + t^8.74/(g1^4*g2^4) + 2*g1^3*g2^3*t^8.87 - t^8.89/g2^3 - 7*g1*g2*t^8.96 - t^8.98/(g1^2*g2^5) + t^8.57/y^2 - t^3.86/y - t^4.71/y - t^6.04/(g1*g2*y) - t^6.43/y - (2*g1*g2*t^6.82)/y - t^6.9/(g1*g2*y) - t^7.29/y - (2*g1*g2*t^7.67)/y + (2*t^8.14)/y - t^8.23/(g1^2*g2^2*y) + (g1*g2*t^8.53)/y - (3*t^8.61)/(g1*g2*y) + (g1^2*g2^2*t^8.92)/y - t^3.86*y - t^4.71*y - (t^6.04*y)/(g1*g2) - t^6.43*y - 2*g1*g2*t^6.82*y - (t^6.9*y)/(g1*g2) - t^7.29*y - 2*g1*g2*t^7.67*y + 2*t^8.14*y - (t^8.23*y)/(g1^2*g2^2) + g1*g2*t^8.53*y - (3*t^8.61*y)/(g1*g2) + g1^2*g2^2*t^8.92*y + t^8.57*y^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 |
|---|---|---|---|---|---|---|---|---|---|
| 57689 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ | 1.4957 | 1.7262 | 0.8665 | [X:[], M:[0.9832, 0.6815], q:[0.5141, 0.4805], qb:[0.5027, 0.4914], phi:[0.3352]] | t^2.01 + t^2.04 + t^2.92 + 2*t^2.95 + 2*t^3.02 + t^3.92 + 2*t^4.02 + 2*t^4.06 + t^4.09 + 2*t^4.93 + 4*t^4.96 + 2*t^4.99 + 3*t^5.03 + 3*t^5.06 + t^5.43 + t^5.46 + t^5.5 + t^5.53 + t^5.83 + 2*t^5.87 + 2*t^5.9 + 3*t^5.93 + 4*t^5.97 - 4*t^6. - t^4.01/y - t^5.01/y - t^4.01*y - t^5.01*y | detail |