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 |
|---|---|---|---|---|---|---|---|---|---|
| 61028 | SU3adj1nf2 | ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{2}^{2}$ | 0.9738 | 1.1873 | 0.8202 | [X:[1.5847, 1.4153, 1.5847, 1.4153], M:[0.9153, 0.6695], q:[0.1384, 0.3079], qb:[0.2768, 0.2768], phi:[0.5]] | [X:[[-3], [3], [-3], [3]], M:[[3], [-6]], q:[[1], [-5]], qb:[[2], [2]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{2}$, ${ }X_{4}$, ${ }\phi_{1}^{3}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }X_{3}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }M_{2}\phi_{1}q_{1}q_{2}^{2}$ | ${}\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1 | t^2.01 + 3*t^2.75 + t^3. + 2*t^3.25 + t^3.76 + t^3.99 + t^4.02 + 4*t^4.25 + t^4.5 + 8*t^4.75 + t^5.01 + 3*t^5.26 + 7*t^5.49 + 2*t^5.75 + t^5.77 + t^6. + t^6.03 + 4*t^6.25 + 2*t^6.51 + t^6.74 + 9*t^6.76 + 14*t^6.99 + 3*t^7.02 + 2*t^7.25 + 4*t^7.27 + 21*t^7.5 + t^7.53 + 4*t^7.75 + t^7.78 + t^7.98 + 9*t^8.01 + t^8.03 + 9*t^8.24 + 4*t^8.26 + 8*t^8.49 + 5*t^8.52 - 10*t^8.75 + 8*t^8.77 - t^4.5/y - t^6./y - t^6.51/y - t^7.25/y + t^7.5/y + (4*t^7.75)/y + (2*t^8.26)/y + (4*t^8.49)/y - t^8.52/y - (2*t^8.75)/y + t^8.77/y - t^4.5*y - t^6.*y - t^6.51*y - t^7.25*y + t^7.5*y + 4*t^7.75*y + 2*t^8.26*y + 4*t^8.49*y - t^8.52*y - 2*t^8.75*y + t^8.77*y | t^2.01/g1^6 + 3*g1^3*t^2.75 + t^3. + (2*t^3.25)/g1^3 + t^3.76/g1^9 + g1^6*t^3.99 + t^4.02/g1^12 + 4*g1^3*t^4.25 + t^4.5 + (8*t^4.75)/g1^3 + t^5.01/g1^6 + (3*t^5.26)/g1^9 + 7*g1^6*t^5.49 + 2*g1^3*t^5.75 + t^5.77/g1^15 + t^6. + t^6.03/g1^18 + (4*t^6.25)/g1^3 + (2*t^6.51)/g1^6 + g1^9*t^6.74 + (9*t^6.76)/g1^9 + 14*g1^6*t^6.99 + (3*t^7.02)/g1^12 + 2*g1^3*t^7.25 + (4*t^7.27)/g1^15 + 21*t^7.5 + t^7.53/g1^18 + (4*t^7.75)/g1^3 + t^7.78/g1^21 + g1^12*t^7.98 + (9*t^8.01)/g1^6 + t^8.03/g1^24 + 9*g1^9*t^8.24 + (4*t^8.26)/g1^9 + 8*g1^6*t^8.49 + (5*t^8.52)/g1^12 - 10*g1^3*t^8.75 + (8*t^8.77)/g1^15 - t^4.5/y - t^6./y - t^6.51/(g1^6*y) - (g1^3*t^7.25)/y + t^7.5/y + (4*t^7.75)/(g1^3*y) + (2*t^8.26)/(g1^9*y) + (4*g1^6*t^8.49)/y - t^8.52/(g1^12*y) - (2*g1^3*t^8.75)/y + t^8.77/(g1^15*y) - t^4.5*y - t^6.*y - (t^6.51*y)/g1^6 - g1^3*t^7.25*y + t^7.5*y + (4*t^7.75*y)/g1^3 + (2*t^8.26*y)/g1^9 + 4*g1^6*t^8.49*y - (t^8.52*y)/g1^12 - 2*g1^3*t^8.75*y + (t^8.77*y)/g1^15 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 58628 | SU3adj1nf2 | ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.9786 | 1.1906 | 0.8219 | [X:[1.5248, 1.392, 1.608, 1.4752], M:[0.892, 0.7159], q:[0.1584, 0.2912], qb:[0.3168, 0.2336], phi:[0.5]] | t^2.15 + 2*t^2.68 + t^2.93 + t^3. + t^3.07 + t^3.32 + t^3.72 + t^4.1 + 2*t^4.18 + t^4.3 + 2*t^4.43 + t^4.5 + 2*t^4.57 + 5*t^4.82 + t^5.07 + t^5.15 + 2*t^5.22 + 4*t^5.35 + t^5.47 + 2*t^5.6 + t^5.68 + t^5.75 + t^5.85 + t^5.87 + t^5.93 - t^6. - t^4.5/y - t^6./y - t^4.5*y - t^6.*y | detail |