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 |
|---|---|---|---|---|---|---|---|---|---|
| 61070 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ | 1.4102 | 1.6301 | 0.8651 | [X:[], M:[0.8963, 1.2642], q:[0.3835, 0.4972], qb:[0.5596, 0.3523], phi:[0.3679]] | [X:[], M:[[9], [6]], q:[[-14], [34]], qb:[[-10], [8]], phi:[[-3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{5}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${}M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$ | 1 | t^2.21 + t^2.55 + t^2.69 + t^2.83 + t^3.17 + t^3.31 + t^3.65 + t^3.79 + t^3.93 + t^4.27 + 2*t^4.41 + 2*t^4.76 + 3*t^4.9 + 2*t^5.04 + t^5.1 + 2*t^5.24 + 3*t^5.38 + 3*t^5.52 + t^5.72 + 3*t^5.86 + t^6. + 2*t^6.14 + t^6.2 + 3*t^6.34 + 5*t^6.48 + 5*t^6.62 + t^6.76 + 2*t^6.82 + 5*t^6.96 + 5*t^7.1 + 3*t^7.24 + 3*t^7.3 + 6*t^7.44 + 7*t^7.59 + t^7.65 + 5*t^7.73 + 3*t^7.79 + t^7.87 + 6*t^7.93 + 8*t^8.07 + 5*t^8.21 + t^8.27 + 3*t^8.35 + 4*t^8.41 + 6*t^8.55 + 5*t^8.69 + t^8.75 + 5*t^8.83 + 4*t^8.89 + t^8.97 - t^4.1/y - t^5.21/y - t^6.31/y - t^6.65/y - t^6.79/y - t^6.93/y - t^7.27/y - t^7.41/y + t^8.24/y + t^8.38/y + t^8.72/y + t^8.86/y - t^4.1*y - t^5.21*y - t^6.31*y - t^6.65*y - t^6.79*y - t^6.93*y - t^7.27*y - t^7.41*y + t^8.24*y + t^8.38*y + t^8.72*y + t^8.86*y | t^2.21/g1^6 + g1^42*t^2.55 + g1^9*t^2.69 + t^2.83/g1^24 + g1^24*t^3.17 + t^3.31/g1^9 + g1^39*t^3.65 + g1^6*t^3.79 + t^3.93/g1^27 + g1^21*t^4.27 + (2*t^4.41)/g1^12 + 2*g1^36*t^4.76 + 3*g1^3*t^4.9 + (2*t^5.04)/g1^30 + g1^84*t^5.1 + 2*g1^51*t^5.24 + 3*g1^18*t^5.38 + (3*t^5.52)/g1^15 + g1^66*t^5.72 + 3*g1^33*t^5.86 + t^6. + (2*t^6.14)/g1^33 + g1^81*t^6.2 + 3*g1^48*t^6.34 + 5*g1^15*t^6.48 + (5*t^6.62)/g1^18 + t^6.76/g1^51 + 2*g1^63*t^6.82 + 5*g1^30*t^6.96 + (5*t^7.1)/g1^3 + (3*t^7.24)/g1^36 + 3*g1^78*t^7.3 + 6*g1^45*t^7.44 + 7*g1^12*t^7.59 + g1^126*t^7.65 + (5*t^7.73)/g1^21 + 3*g1^93*t^7.79 + t^7.87/g1^54 + 6*g1^60*t^7.93 + 8*g1^27*t^8.07 + (5*t^8.21)/g1^6 + g1^108*t^8.27 + (3*t^8.35)/g1^39 + 4*g1^75*t^8.41 + 6*g1^42*t^8.55 + 5*g1^9*t^8.69 + g1^123*t^8.75 + (5*t^8.83)/g1^24 + 4*g1^90*t^8.89 + t^8.97/g1^57 - t^4.1/(g1^3*y) - t^5.21/(g1^6*y) - t^6.31/(g1^9*y) - (g1^39*t^6.65)/y - (g1^6*t^6.79)/y - t^6.93/(g1^27*y) - (g1^21*t^7.27)/y - t^7.41/(g1^12*y) + (g1^51*t^8.24)/y + (g1^18*t^8.38)/y + (g1^66*t^8.72)/y + (g1^33*t^8.86)/y - (t^4.1*y)/g1^3 - (t^5.21*y)/g1^6 - (t^6.31*y)/g1^9 - g1^39*t^6.65*y - g1^6*t^6.79*y - (t^6.93*y)/g1^27 - g1^21*t^7.27*y - (t^7.41*y)/g1^12 + g1^51*t^8.24*y + g1^18*t^8.38*y + g1^66*t^8.72*y + g1^33*t^8.86*y |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 59460 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1.4298 | 1.6661 | 0.8582 | [X:[], M:[0.8968], q:[0.3828, 0.499], qb:[0.5591, 0.3527], phi:[0.3677]] | 2*t^2.21 + t^2.55 + t^2.69 + t^2.83 + t^3.17 + t^3.31 + t^3.66 + t^3.93 + t^4.28 + 4*t^4.41 + 3*t^4.76 + 4*t^4.9 + 3*t^5.03 + t^5.11 + 2*t^5.25 + 4*t^5.38 + 4*t^5.52 + t^5.73 + 4*t^5.86 - t^4.1/y - t^5.21/y - t^4.1*y - t^5.21*y | detail |