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 |
|---|---|---|---|---|---|---|---|---|---|
| 61238 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ | 1.1906 | 1.421 | 0.8379 | [X:[1.6], M:[0.7567, 1.1567, 0.8], q:[0.2144, 0.5712], qb:[0.6288, 0.1856], phi:[0.4]] | [X:[[0, 0]], M:[[-1, 1], [-1, 1], [0, 0]], q:[[0, -1], [-1, 0]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{2}^{2}$ | ${}M_{3}\phi_{1}^{3}$, ${ }M_{3}\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}^{2}\tilde{q}_{2}^{2}$ | 2 | 2*t^2.27 + 3*t^2.4 + 2*t^3.47 + 2*t^3.6 + 2*t^4.2 + 3*t^4.54 + 6*t^4.67 + 8*t^4.8 + 2*t^5.27 + 2*t^5.4 + 2*t^5.53 + 4*t^5.74 + 9*t^5.87 + 2*t^6. - t^6.13 + 4*t^6.47 + 6*t^6.6 + 4*t^6.81 + 12*t^6.94 + 17*t^7.07 + 14*t^7.2 - 3*t^7.33 + 4*t^7.54 + 10*t^7.67 + 6*t^7.8 + 2*t^7.93 + 6*t^8.01 + 16*t^8.14 + 15*t^8.27 - 5*t^8.53 + 10*t^8.74 + 14*t^8.87 - t^4.2/y - t^5.4/y - (2*t^6.47)/y - (2*t^6.6)/y + t^7.54/y + (3*t^7.67)/y + t^7.93/y + t^8.74/y + (5*t^8.87)/y - t^4.2*y - t^5.4*y - 2*t^6.47*y - 2*t^6.6*y + t^7.54*y + 3*t^7.67*y + t^7.93*y + t^8.74*y + 5*t^8.87*y | (2*g2*t^2.27)/g1 + 3*t^2.4 + (2*g2*t^3.47)/g1 + 2*t^3.6 + t^4.2/(g1*g2^2) + g1*g2^2*t^4.2 + (3*g2^2*t^4.54)/g1^2 + (6*g2*t^4.67)/g1 + 8*t^4.8 + t^5.27/(g1^2*g2) + g2^3*t^5.27 + t^5.4/(g1*g2^2) + g1*g2^2*t^5.4 + t^5.53/g2^3 + g1^2*g2*t^5.53 + (4*g2^2*t^5.74)/g1^2 + (9*g2*t^5.87)/g1 + 2*t^6. - (g1*t^6.13)/g2 + (2*t^6.47)/(g1^2*g2) + 2*g2^3*t^6.47 + (3*t^6.6)/(g1*g2^2) + 3*g1*g2^2*t^6.6 + (4*g2^3*t^6.81)/g1^3 + (12*g2^2*t^6.94)/g1^2 + (17*g2*t^7.07)/g1 + 14*t^7.2 - (3*g1*t^7.33)/g2 + (2*t^7.54)/g1^3 + (2*g2^4*t^7.54)/g1 + (5*t^7.67)/(g1^2*g2) + 5*g2^3*t^7.67 + (3*t^7.8)/(g1*g2^2) + 3*g1*g2^2*t^7.8 + t^7.93/g2^3 + g1^2*g2*t^7.93 + (6*g2^3*t^8.01)/g1^3 + (16*g2^2*t^8.14)/g1^2 + (15*g2*t^8.27)/g1 - 2*t^8.4 + t^8.4/(g1^2*g2^4) + g1^2*g2^4*t^8.4 - (5*g1*t^8.53)/g2 + (5*t^8.74)/g1^3 + (5*g2^4*t^8.74)/g1 + (7*t^8.87)/(g1^2*g2) + 7*g2^3*t^8.87 - t^4.2/y - t^5.4/y - (2*g2*t^6.47)/(g1*y) - (2*t^6.6)/y + (g2^2*t^7.54)/(g1^2*y) + (3*g2*t^7.67)/(g1*y) + (g1*t^7.93)/(g2*y) + (g2^2*t^8.74)/(g1^2*y) + (5*g2*t^8.87)/(g1*y) - t^4.2*y - t^5.4*y - (2*g2*t^6.47*y)/g1 - 2*t^6.6*y + (g2^2*t^7.54*y)/g1^2 + (3*g2*t^7.67*y)/g1 + (g1*t^7.93*y)/g2 + (g2^2*t^8.74*y)/g1^2 + (5*g2*t^8.87*y)/g1 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 58355 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ | 1.1741 | 1.392 | 0.8435 | [X:[1.6], M:[0.7567, 1.1567], q:[0.2144, 0.5712], qb:[0.6288, 0.1856], phi:[0.4]] | 2*t^2.27 + 2*t^2.4 + 2*t^3.47 + 3*t^3.6 + 2*t^4.2 + 3*t^4.54 + 4*t^4.67 + 5*t^4.8 + 2*t^5.27 + 2*t^5.4 + 2*t^5.53 + 4*t^5.74 + 9*t^5.87 + 2*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail |