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 |
|---|---|---|---|---|---|---|---|---|---|
| 55369 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{3}M_{4}$ + ${ }M_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{6}X_{1}$ | 0.5845 | 0.7293 | 0.8015 | [X:[1.3167], M:[0.7083, 1.0, 1.025, 0.975, 0.6833, 0.6833], q:[0.3167, 0.975], qb:[0.6833, 0.6583], phi:[0.3417]] | [X:[[2]], M:[[-5], [0], [-3], [3], [-2], [-2]], q:[[2], [3]], qb:[[-2], [1]], phi:[[-1]]] | 1 | {a: 89779/153600, c: 112019/153600, X1: 79/60, M1: 17/24, M2: 1, M3: 41/40, M4: 39/40, M5: 41/60, M6: 41/60, q1: 19/60, q2: 39/40, qb1: 41/60, qb2: 79/120, phi1: 41/120} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{6}$, ${ }M_{1}$, ${ }M_{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{6}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$ | ${}$ | -3 | 2*t^2.05 + t^2.125 + 2*t^2.925 + t^3. + t^4.025 + 3*t^4.1 + 2*t^4.175 + t^4.25 + t^4.9 + 5*t^4.975 + 3*t^5.05 + t^5.125 + 3*t^5.85 + t^5.925 - 3*t^6. + 5*t^6.15 + 3*t^6.225 + 2*t^6.3 + t^6.375 - t^6.875 + t^6.95 + 7*t^7.025 + 5*t^7.1 + 3*t^7.175 + t^7.25 + t^7.825 + 5*t^7.9 + t^7.975 - 4*t^8.05 - 3*t^8.125 + 5*t^8.2 + 5*t^8.275 + 3*t^8.35 + 2*t^8.425 + t^8.5 + 4*t^8.775 - t^8.85 - 9*t^8.925 - t^4.025/y - (2*t^6.075)/y - t^6.15/y + t^7.1/y + (2*t^7.175)/y + t^7.9/y + (6*t^7.975)/y + (4*t^8.05)/y - (2*t^8.125)/y - (2*t^8.2)/y - t^8.275/y + t^8.85/y + (2*t^8.925)/y - t^4.025*y - 2*t^6.075*y - t^6.15*y + t^7.1*y + 2*t^7.175*y + t^7.9*y + 6*t^7.975*y + 4*t^8.05*y - 2*t^8.125*y - 2*t^8.2*y - t^8.275*y + t^8.85*y + 2*t^8.925*y | (2*t^2.05)/g1^2 + t^2.125/g1^5 + 2*g1^3*t^2.925 + t^3. + t^4.025/g1 + (3*t^4.1)/g1^4 + (2*t^4.175)/g1^7 + t^4.25/g1^10 + g1^4*t^4.9 + 5*g1*t^4.975 + (3*t^5.05)/g1^2 + t^5.125/g1^5 + 3*g1^6*t^5.85 + g1^3*t^5.925 - 3*t^6. + (5*t^6.15)/g1^6 + (3*t^6.225)/g1^9 + (2*t^6.3)/g1^12 + t^6.375/g1^15 - g1^5*t^6.875 + g1^2*t^6.95 + (7*t^7.025)/g1 + (5*t^7.1)/g1^4 + (3*t^7.175)/g1^7 + t^7.25/g1^10 + g1^7*t^7.825 + 5*g1^4*t^7.9 + g1*t^7.975 - (4*t^8.05)/g1^2 - (3*t^8.125)/g1^5 + (5*t^8.2)/g1^8 + (5*t^8.275)/g1^11 + (3*t^8.35)/g1^14 + (2*t^8.425)/g1^17 + t^8.5/g1^20 + 4*g1^9*t^8.775 - g1^6*t^8.85 - 9*g1^3*t^8.925 - t^4.025/(g1*y) - (2*t^6.075)/(g1^3*y) - t^6.15/(g1^6*y) + t^7.1/(g1^4*y) + (2*t^7.175)/(g1^7*y) + (g1^4*t^7.9)/y + (6*g1*t^7.975)/y + (4*t^8.05)/(g1^2*y) - (2*t^8.125)/(g1^5*y) - (2*t^8.2)/(g1^8*y) - t^8.275/(g1^11*y) + (g1^6*t^8.85)/y + (2*g1^3*t^8.925)/y - (t^4.025*y)/g1 - (2*t^6.075*y)/g1^3 - (t^6.15*y)/g1^6 + (t^7.1*y)/g1^4 + (2*t^7.175*y)/g1^7 + g1^4*t^7.9*y + 6*g1*t^7.975*y + (4*t^8.05*y)/g1^2 - (2*t^8.125*y)/g1^5 - (2*t^8.2*y)/g1^8 - (t^8.275*y)/g1^11 + g1^6*t^8.85*y + 2*g1^3*t^8.925*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47017 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{3}M_{4}$ + ${ }M_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}\tilde{q}_{2}$ | 0.5637 | 0.6887 | 0.8185 | [X:[1.3155], M:[0.7113, 1.0, 1.0268, 0.9732, 0.6845], q:[0.3155, 0.9732], qb:[0.6845, 0.6577], phi:[0.3423]] | t^2.054 + t^2.134 + 2*t^2.92 + t^3. + t^3.946 + t^4.027 + t^4.107 + t^4.187 + t^4.268 + t^4.893 + 3*t^4.973 + 2*t^5.054 + t^5.134 + 3*t^5.839 + t^5.92 - 2*t^6. - t^4.027/y - t^4.027*y | detail |