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 |
|---|---|---|---|---|---|---|---|---|---|
| 46184 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | 0.5658 | 0.7265 | 0.7788 | [M:[1.0, 0.7154, 0.8577], q:[0.7856, 0.2144], qb:[0.499, 0.7856], phi:[0.4289]] | [M:[[0], [-8], [-4]], q:[[1], [-1]], qb:[[7], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}^{4}$, ${ }M_{1}M_{3}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ | ${}\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ | 0 | t^2.14 + t^2.146 + 3*t^2.573 + 2*t^3. + t^3.854 + 2*t^4.281 + t^4.287 + t^4.293 + 4*t^4.713 + 3*t^4.719 + 2*t^5.14 + 7*t^5.146 + 4*t^5.573 + t^5.994 + 2*t^6.421 + t^6.427 + t^6.439 + 5*t^6.854 + 2*t^6.86 + 3*t^6.866 + 2*t^7.281 + 7*t^7.287 + 7*t^7.293 + 2*t^7.713 + 11*t^7.719 + 2*t^8.134 - 3*t^8.14 + 4*t^8.146 + 3*t^8.561 - 4*t^8.573 + t^8.585 + 5*t^8.994 - t^4.287/y - t^6.433/y - (2*t^6.86)/y + t^7.287/y + (5*t^7.713)/y + (3*t^7.719)/y + (3*t^8.14)/y + (5*t^8.146)/y + (6*t^8.573)/y - t^8.579/y + t^8.994/y - t^4.287*y - t^6.433*y - 2*t^6.86*y + t^7.287*y + 5*t^7.713*y + 3*t^7.719*y + 3*t^8.14*y + 5*t^8.146*y + 6*t^8.573*y - t^8.579*y + t^8.994*y | g1^6*t^2.14 + t^2.146/g1^8 + (3*t^2.573)/g1^4 + 2*t^3. + g1^8*t^3.854 + 2*g1^12*t^4.281 + t^4.287/g1^2 + t^4.293/g1^16 + 4*g1^2*t^4.713 + (3*t^4.719)/g1^12 + 2*g1^6*t^5.14 + (7*t^5.146)/g1^8 + (4*t^5.573)/g1^4 + g1^14*t^5.994 + 2*g1^18*t^6.421 + g1^4*t^6.427 + t^6.439/g1^24 + 5*g1^8*t^6.854 + (2*t^6.86)/g1^6 + (3*t^6.866)/g1^20 + 2*g1^12*t^7.281 + (7*t^7.287)/g1^2 + (7*t^7.293)/g1^16 + 2*g1^2*t^7.713 + (11*t^7.719)/g1^12 + 2*g1^20*t^8.134 - 3*g1^6*t^8.14 + (4*t^8.146)/g1^8 + 3*g1^24*t^8.561 - (4*t^8.573)/g1^4 + t^8.585/g1^32 + 5*g1^14*t^8.994 - t^4.287/(g1^2*y) - t^6.433/(g1^10*y) - (2*t^6.86)/(g1^6*y) + t^7.287/(g1^2*y) + (5*g1^2*t^7.713)/y + (3*t^7.719)/(g1^12*y) + (3*g1^6*t^8.14)/y + (5*t^8.146)/(g1^8*y) + (6*t^8.573)/(g1^4*y) - t^8.579/(g1^18*y) + (g1^14*t^8.994)/y - (t^4.287*y)/g1^2 - (t^6.433*y)/g1^10 - (2*t^6.86*y)/g1^6 + (t^7.287*y)/g1^2 + 5*g1^2*t^7.713*y + (3*t^7.719*y)/g1^12 + 3*g1^6*t^8.14*y + (5*t^8.146*y)/g1^8 + (6*t^8.573*y)/g1^4 - (t^8.579*y)/g1^18 + g1^14*t^8.994*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 |
|---|---|---|---|---|---|---|---|---|
| 46366 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ | 0.5861 | 0.7654 | 0.7658 | [M:[1.0, 0.7055, 0.8528, 0.7055], q:[0.7868, 0.2132], qb:[0.5077, 0.7868], phi:[0.4264]] | 2*t^2.117 + t^2.163 + 3*t^2.558 + 2*t^3. + 3*t^4.233 + 2*t^4.279 + 2*t^4.325 + 6*t^4.675 + 4*t^4.721 + 9*t^5.117 + 2*t^5.163 + 4*t^5.558 - t^6. - t^4.279/y - t^4.279*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46049 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.614 | 0.7856 | 0.7817 | [M:[1.0, 0.8753, 0.7244], q:[0.7656, 0.2344], qb:[0.5724, 0.5523], phi:[0.4688]] | t^2.173 + t^2.36 + t^2.42 + t^2.626 + 2*t^2.813 + t^3. + t^3.767 + t^3.954 + t^4.014 + t^4.346 + t^4.533 + t^4.593 + 2*t^4.72 + 2*t^4.78 + t^4.799 + 2*t^4.841 + 2*t^4.986 + 3*t^5.173 + 2*t^5.233 + t^5.252 + t^5.36 + t^5.42 + 2*t^5.439 + 4*t^5.626 + t^5.813 - 3*t^6. - t^4.407/y - t^4.407*y | detail |