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 |
|---|---|---|---|---|---|---|---|---|---|
| 60637 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ | 1.3885 | 1.5721 | 0.8832 | [X:[1.3541], M:[0.7763, 1.1615], q:[0.367, 0.69], qb:[0.4715, 0.5337], phi:[0.323]] | [X:[[0, 4]], M:[[0, -11], [0, -1]], q:[[-1, 13], [-1, 11]], qb:[[1, -12], [1, 0]], phi:[[0, -2]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{6}$, ${ }M_{1}q_{2}\tilde{q}_{1}$ | ${}$ | -4 | t^2.33 + t^2.7 + t^2.91 + 3*t^3.48 + t^3.67 + t^4.06 + 2*t^4.45 + 2*t^4.64 + t^4.66 + 2*t^5.24 + 2*t^5.4 + t^5.42 + t^5.59 + 2*t^5.61 + 3*t^5.81 - 4*t^6. + 2*t^6.19 + 3*t^6.21 + 2*t^6.37 + 4*t^6.39 + t^6.55 + t^6.58 + t^6.76 + t^6.78 - t^6.95 + 4*t^6.97 + t^6.99 + t^7.15 + 4*t^7.16 + 2*t^7.18 + 4*t^7.34 + 2*t^7.36 + t^7.52 + 4*t^7.55 + t^7.56 - t^7.57 + t^7.71 - 2*t^7.76 - 2*t^7.91 + 5*t^7.94 + t^8.11 + 8*t^8.12 + 3*t^8.14 + 2*t^8.15 + t^8.29 + 5*t^8.31 - 2*t^8.33 + t^8.49 + t^8.52 - 6*t^8.7 + 4*t^8.72 + 2*t^8.89 + 6*t^8.91 + t^8.91/y^2 - t^3.97/y - t^4.94/y - t^6.3/y - t^6.67/y - t^6.88/y - t^7.27/y - (2*t^7.45)/y - t^7.64/y - t^7.84/y + t^8.03/y + t^8.24/y - (3*t^8.42)/y - t^8.63/y + (3*t^8.81)/y - t^3.97*y - t^4.94*y - t^6.3*y - t^6.67*y - t^6.88*y - t^7.27*y - 2*t^7.45*y - t^7.64*y - t^7.84*y + t^8.03*y + t^8.24*y - 3*t^8.42*y - t^8.63*y + 3*t^8.81*y + t^8.91*y^2 | t^2.33/g2^11 + g2^13*t^2.7 + t^2.91/g2^6 + (3*t^3.48)/g2 + g2^11*t^3.67 + g2^4*t^4.06 + (2*t^4.45)/g2^3 + 2*g2^9*t^4.64 + t^4.66/g2^22 + t^5.24/g2^17 + (g2^35*t^5.24)/g1^3 + (g1^3*t^5.4)/g2^26 + g2^26*t^5.4 + t^5.42/g2^5 + (g1^3*t^5.59)/g2^14 + 2*g2^7*t^5.61 + (3*t^5.81)/g2^12 - 4*t^6. + 2*g2^12*t^6.19 + (3*g2^33*t^6.21)/g1^3 + (g1^3*t^6.37)/g2^28 + g2^24*t^6.37 + (4*t^6.39)/g2^7 + (g1^3*t^6.55)/g2^16 + g2^5*t^6.58 + g2^17*t^6.76 + t^6.78/g2^14 - (g1^3*t^6.95)/g2^23 + (4*t^6.97)/g2^2 + t^6.99/g2^33 + (g1^3*t^7.15)/g2^42 + 4*g2^10*t^7.16 + (2*g2^31*t^7.18)/g1^3 + (g1^3*t^7.34)/g2^30 + 3*g2^22*t^7.34 + (2*t^7.36)/g2^9 + (g1^3*t^7.52)/g2^18 + 4*g2^3*t^7.55 + t^7.56/g2^28 - (g2^24*t^7.57)/g1^3 + (g1^3*t^7.71)/g2^6 - (2*g2^36*t^7.76)/g1^3 - (2*g1^3*t^7.91)/g2^25 + (4*t^7.94)/g2^4 + (g2^48*t^7.94)/g1^3 + g2^39*t^8.11 + 8*g2^8*t^8.12 + (3*t^8.14)/g2^23 + (2*g2^29*t^8.15)/g1^3 + (g1^3*t^8.29)/g2 + (g1^3*t^8.31)/g2^32 + 4*g2^20*t^8.31 - (2*t^8.33)/g2^11 + (g1^3*t^8.49)/g2^20 + g2*t^8.52 - (g1^3*t^8.7)/g2^39 - 5*g2^13*t^8.7 + (4*t^8.72)/g2^18 + 2*g2^25*t^8.89 + (2*t^8.91)/g2^6 + (4*g2^46*t^8.91)/g1^3 + t^8.91/(g2^6*y^2) - t^3.97/(g2^2*y) - t^4.94/(g2^4*y) - t^6.3/(g2^13*y) - (g2^11*t^6.67)/y - t^6.88/(g2^8*y) - t^7.27/(g2^15*y) - (2*t^7.45)/(g2^3*y) - (g2^9*t^7.64)/y - t^7.84/(g2^10*y) + (g2^2*t^8.03)/y + t^8.24/(g2^17*y) - (3*t^8.42)/(g2^5*y) - t^8.63/(g2^24*y) + (3*t^8.81)/(g2^12*y) - (t^3.97*y)/g2^2 - (t^4.94*y)/g2^4 - (t^6.3*y)/g2^13 - g2^11*t^6.67*y - (t^6.88*y)/g2^8 - (t^7.27*y)/g2^15 - (2*t^7.45*y)/g2^3 - g2^9*t^7.64*y - (t^7.84*y)/g2^10 + g2^2*t^8.03*y + (t^8.24*y)/g2^17 - (3*t^8.42*y)/g2^5 - (t^8.63*y)/g2^24 + (3*t^8.81*y)/g2^12 + (t^8.91*y^2)/g2^6 |
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 57731 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.4024 | 1.5963 | 0.8785 | [X:[1.3532], M:[0.7786], q:[0.3662, 0.6896], qb:[0.4721, 0.5317], phi:[0.3234]] | t^2.34 + t^2.51 + t^2.69 + t^2.91 + 2*t^3.49 + t^3.66 + t^4.06 + 2*t^4.46 + 2*t^4.63 + t^4.67 + t^4.85 + t^5.03 + t^5.21 + t^5.24 + t^5.25 + t^5.39 + t^5.4 + 2*t^5.43 + t^5.58 + 2*t^5.6 + 2*t^5.82 - 2*t^6. - t^3.97/y - t^4.94/y - t^3.97*y - t^4.94*y | detail |