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 |
|---|---|---|---|---|---|---|---|---|---|
| 61086 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ | 1.3611 | 1.5748 | 0.8643 | [X:[], M:[1.1801, 1.2024, 1.1976], q:[0.4117, 0.3942], qb:[0.4082, 0.3859], phi:[0.4]] | [X:[], M:[[1, 2], [2, 1], [-2, -1]], q:[[-2, -2], [1, 1]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.34 + t^2.4 + 2*t^3.54 + 2*t^3.59 + t^3.6 + 2*t^3.61 + t^3.66 + t^4.68 + 3*t^4.74 + t^4.79 + 2*t^4.8 + 2*t^4.81 + t^4.85 + t^4.86 + 2*t^5.88 + t^5.93 + 4*t^5.94 + t^5.95 + 2*t^5.99 - t^6. + 3*t^6.01 + t^6.06 - t^6.07 + t^7.02 + t^7.07 + 6*t^7.08 + 4*t^7.13 + 6*t^7.14 + 5*t^7.15 + 5*t^7.19 + 6*t^7.2 + 7*t^7.21 + 3*t^7.25 + 2*t^7.27 + t^7.3 + t^7.32 + 2*t^8.22 + t^8.27 + 7*t^8.28 + t^8.29 + 5*t^8.33 + 3*t^8.34 + 6*t^8.35 + 5*t^8.39 + 3*t^8.4 + 6*t^8.41 + 3*t^8.45 + t^8.46 + t^8.47 + t^8.52 - t^4.2/y - t^5.4/y - t^6.54/y - t^6.6/y - t^7.74/y - t^7.79/y - t^7.8/y - t^7.81/y + t^8.88/y + (2*t^8.93)/y + (2*t^8.95)/y - t^4.2*y - t^5.4*y - t^6.54*y - t^6.6*y - t^7.74*y - t^7.79*y - t^7.8*y - t^7.81*y + t^8.88*y + 2*t^8.93*y + 2*t^8.95*y | g1*g2^2*t^2.34 + t^2.4 + 2*g1*g2^2*t^3.54 + (2*t^3.59)/(g1^2*g2) + t^3.6 + 2*g1^2*g2*t^3.61 + t^3.66/(g1*g2^2) + g1^2*g2^4*t^4.68 + 3*g1*g2^2*t^4.74 + t^4.79/(g1^2*g2) + 2*t^4.8 + 2*g1^2*g2*t^4.81 + t^4.85/(g1^3*g2^3) + t^4.86/(g1*g2^2) + 2*g1^2*g2^4*t^5.88 + (g2*t^5.93)/g1 + 4*g1*g2^2*t^5.94 + g1^3*g2^3*t^5.95 + (2*t^5.99)/(g1^2*g2) - t^6. + 3*g1^2*g2*t^6.01 + t^6.06/(g1*g2^2) - (g1*t^6.07)/g2 + g1^3*g2^6*t^7.02 + g2^3*t^7.07 + 6*g1^2*g2^4*t^7.08 + (4*g2*t^7.13)/g1 + 6*g1*g2^2*t^7.14 + 5*g1^3*g2^3*t^7.15 + (3*t^7.19)/(g1^4*g2^2) + (2*t^7.19)/(g1^2*g2) + 6*t^7.2 + 4*g1^2*g2*t^7.21 + 3*g1^4*g2^2*t^7.21 + (3*t^7.25)/(g1^3*g2^3) + g1^3*t^7.27 + (g1*t^7.27)/g2 + t^7.3/(g1^6*g2^6) + t^7.32/(g1^2*g2^4) + 2*g1^3*g2^6*t^8.22 + g2^3*t^8.27 + 7*g1^2*g2^4*t^8.28 + g1^4*g2^5*t^8.29 + (5*g2*t^8.33)/g1 + 3*g1*g2^2*t^8.34 + 6*g1^3*g2^3*t^8.35 + (2*t^8.39)/(g1^4*g2^2) + (3*t^8.39)/(g1^2*g2) + 3*t^8.4 + 3*g1^2*g2*t^8.41 + 3*g1^4*g2^2*t^8.41 + t^8.45/(g1^5*g2^4) + (2*t^8.45)/(g1^3*g2^3) + t^8.46/(g1*g2^2) + (g1*t^8.47)/g2 + t^8.52/(g1^2*g2^4) - t^4.2/y - t^5.4/y - (g1*g2^2*t^6.54)/y - t^6.6/y - (g1*g2^2*t^7.74)/y - t^7.79/(g1^2*g2*y) - t^7.8/y - (g1^2*g2*t^7.81)/y + (g1^2*g2^4*t^8.88)/y + (2*g2*t^8.93)/(g1*y) + (2*g1^3*g2^3*t^8.95)/y - t^4.2*y - t^5.4*y - g1*g2^2*t^6.54*y - t^6.6*y - g1*g2^2*t^7.74*y - (t^7.79*y)/(g1^2*g2) - t^7.8*y - g1^2*g2*t^7.81*y + g1^2*g2^4*t^8.88*y + (2*g2*t^8.93*y)/g1 + 2*g1^3*g2^3*t^8.95*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 |
|---|---|---|---|---|---|---|---|---|---|
| 60043 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ | 1.3781 | 1.6053 | 0.8584 | [X:[], M:[1.1821, 1.1821], q:[0.4239, 0.388], qb:[0.394, 0.394], phi:[0.4]] | 2*t^2.35 + t^2.4 + 4*t^3.55 + t^3.6 + 2*t^3.65 + 3*t^4.69 + 6*t^4.75 + 2*t^4.8 + 2*t^4.85 + t^4.91 + 7*t^5.89 + 8*t^5.95 - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail |