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 |
|---|---|---|---|---|---|---|---|---|---|
| 61089 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ | 1.3917 | 1.6123 | 0.8632 | [X:[], M:[0.8941, 1.2628], q:[0.4027, 0.6144], qb:[0.3346, 0.4367], phi:[0.3686]] | [X:[], M:[[9], [6]], q:[[13], [-5]], qb:[[-19], [29]], phi:[[-3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}M_{2}q_{1}\tilde{q}_{1}$ | 0 | t^2.21 + t^2.52 + t^2.68 + t^2.85 + t^3.15 + t^3.32 + t^3.62 + t^3.79 + t^3.95 + t^4.26 + 3*t^4.42 + 3*t^4.73 + t^4.89 + t^5.04 + 2*t^5.06 + t^5.2 + 4*t^5.36 + 3*t^5.53 + t^5.67 + 4*t^5.84 + t^6.14 + 2*t^6.16 + 2*t^6.31 + t^6.33 + 4*t^6.47 + 6*t^6.64 + 2*t^6.78 + 10*t^6.94 + 2*t^7.11 + 5*t^7.25 + 4*t^7.27 + 3*t^7.41 + t^7.55 + 9*t^7.58 + t^7.72 + 4*t^7.74 + 6*t^7.88 + 10*t^8.05 + t^8.19 + t^8.21 + 6*t^8.35 + 5*t^8.38 + 2*t^8.52 + t^8.54 + t^8.66 + 8*t^8.68 + 2*t^8.82 + 7*t^8.85 + 9*t^8.99 - t^4.11/y - t^5.21/y - t^6.32/y - t^6.62/y - t^6.79/y - t^6.95/y - t^7.26/y - t^7.42/y + t^8.2/y + t^8.36/y + t^8.67/y + t^8.84/y - t^4.11*y - t^5.21*y - t^6.32*y - t^6.62*y - t^6.79*y - t^6.95*y - t^7.26*y - t^7.42*y + t^8.2*y + t^8.36*y + t^8.67*y + t^8.84*y | t^2.21/g1^6 + g1^42*t^2.52 + g1^9*t^2.68 + t^2.85/g1^24 + g1^24*t^3.15 + t^3.32/g1^9 + g1^39*t^3.62 + g1^6*t^3.79 + t^3.95/g1^27 + g1^21*t^4.26 + (3*t^4.42)/g1^12 + 3*g1^36*t^4.73 + g1^3*t^4.89 + g1^84*t^5.04 + (2*t^5.06)/g1^30 + g1^51*t^5.2 + 4*g1^18*t^5.36 + (3*t^5.53)/g1^15 + g1^66*t^5.67 + 4*g1^33*t^5.84 + g1^81*t^6.14 + (2*t^6.16)/g1^33 + 2*g1^48*t^6.31 + t^6.33/g1^66 + 4*g1^15*t^6.47 + (6*t^6.64)/g1^18 + 2*g1^63*t^6.78 + 10*g1^30*t^6.94 + (2*t^7.11)/g1^3 + 5*g1^78*t^7.25 + (4*t^7.27)/g1^36 + 3*g1^45*t^7.41 + g1^126*t^7.55 + 9*g1^12*t^7.58 + g1^93*t^7.72 + (4*t^7.74)/g1^21 + 6*g1^60*t^7.88 + 10*g1^27*t^8.05 + g1^108*t^8.19 + t^8.21/g1^6 + 6*g1^75*t^8.35 + (5*t^8.38)/g1^39 + 2*g1^42*t^8.52 + t^8.54/g1^72 + g1^123*t^8.66 + 8*g1^9*t^8.68 + 2*g1^90*t^8.82 + (7*t^8.85)/g1^24 + 9*g1^57*t^8.99 - t^4.11/(g1^3*y) - t^5.21/(g1^6*y) - t^6.32/(g1^9*y) - (g1^39*t^6.62)/y - (g1^6*t^6.79)/y - t^6.95/(g1^27*y) - (g1^21*t^7.26)/y - t^7.42/(g1^12*y) + (g1^51*t^8.2)/y + (g1^18*t^8.36)/y + (g1^66*t^8.67)/y + (g1^33*t^8.84)/y - (t^4.11*y)/g1^3 - (t^5.21*y)/g1^6 - (t^6.32*y)/g1^9 - g1^39*t^6.62*y - g1^6*t^6.79*y - (t^6.95*y)/g1^27 - g1^21*t^7.26*y - (t^7.42*y)/g1^12 + g1^51*t^8.2*y + g1^18*t^8.36*y + g1^66*t^8.67*y + g1^33*t^8.84*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57896 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.4103 | 1.6303 | 0.865 | [X:[], M:[0.8959, 1.264], q:[0.3474, 0.5555], qb:[0.3887, 0.5003], phi:[0.368]] | t^2.21 + t^2.54 + t^2.69 + t^2.83 + t^3.17 + t^3.31 + t^3.65 + t^3.79 + t^3.94 + t^4.27 + 2*t^4.42 + 2*t^4.75 + t^4.85 + t^4.9 + t^4.94 + 2*t^5.04 + t^5.09 + t^5.23 + t^5.27 + 3*t^5.38 + t^5.48 + 2*t^5.52 + t^5.71 + 3*t^5.86 + t^5.96 - t^6. - t^4.1/y - t^5.21/y - t^4.1*y - t^5.21*y | detail |