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 |
|---|---|---|---|---|---|---|---|---|---|
| 46213 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ | 0.5415 | 0.6866 | 0.7886 | [M:[0.6781, 1.1494, 0.977], q:[0.2989, 1.023], qb:[0.5517, 0.4253], phi:[0.4253]] | [M:[[11], [-2], [7]], q:[[-4], [-7]], qb:[[6], [1]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{2}^{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | -1 | t^2.034 + t^2.172 + t^2.552 + 2*t^2.931 + 2*t^3.448 + t^3.828 + t^4.069 + t^4.207 + 2*t^4.345 + t^4.586 + 2*t^4.724 + 2*t^4.965 + 2*t^5.103 + 3*t^5.483 + t^5.621 + 4*t^5.862 - t^6. + t^6.103 + t^6.241 + 4*t^6.379 + t^6.62 + 3*t^6.758 + t^6.897 + 2*t^6.999 + 2*t^7.138 + 3*t^7.276 - t^7.414 + 3*t^7.517 + 3*t^7.655 + 4*t^7.896 + t^8.034 + t^8.137 - 2*t^8.172 + t^8.275 + 5*t^8.413 - t^8.552 + t^8.655 + 7*t^8.793 - 4*t^8.931 - t^4.276/y - t^6.31/y + t^7.345/y + t^7.586/y + t^7.724/y + (2*t^7.965)/y + (2*t^8.103)/y + t^8.242/y - t^8.344/y + (4*t^8.483)/y + (2*t^8.621)/y + (2*t^8.862)/y - t^4.276*y - t^6.31*y + t^7.345*y + t^7.586*y + t^7.724*y + 2*t^7.965*y + 2*t^8.103*y + t^8.242*y - t^8.344*y + 4*t^8.483*y + 2*t^8.621*y + 2*t^8.862*y | g1^11*t^2.034 + t^2.172/g1^3 + g1^2*t^2.552 + 2*g1^7*t^2.931 + (2*t^3.448)/g1^2 + g1^3*t^3.828 + g1^22*t^4.069 + g1^8*t^4.207 + (2*t^4.345)/g1^6 + g1^13*t^4.586 + (2*t^4.724)/g1 + 2*g1^18*t^4.965 + 2*g1^4*t^5.103 + 3*g1^9*t^5.483 + t^5.621/g1^5 + 4*g1^14*t^5.862 - t^6. + g1^33*t^6.103 + g1^19*t^6.241 + 4*g1^5*t^6.379 + g1^24*t^6.62 + 3*g1^10*t^6.758 + t^6.897/g1^4 + 2*g1^29*t^6.999 + 2*g1^15*t^7.138 + 3*g1*t^7.276 - t^7.414/g1^13 + 3*g1^20*t^7.517 + 3*g1^6*t^7.655 + 4*g1^25*t^7.896 + g1^11*t^8.034 + g1^44*t^8.137 - (2*t^8.172)/g1^3 + g1^30*t^8.275 + 5*g1^16*t^8.413 - g1^2*t^8.552 + g1^35*t^8.655 + 7*g1^21*t^8.793 - 4*g1^7*t^8.931 - (g1*t^4.276)/y - (g1^12*t^6.31)/y + t^7.345/(g1^6*y) + (g1^13*t^7.586)/y + t^7.724/(g1*y) + (2*g1^18*t^7.965)/y + (2*g1^4*t^8.103)/y + t^8.242/(g1^10*y) - (g1^23*t^8.344)/y + (4*g1^9*t^8.483)/y + (2*t^8.621)/(g1^5*y) + (2*g1^14*t^8.862)/y - g1*t^4.276*y - g1^12*t^6.31*y + (t^7.345*y)/g1^6 + g1^13*t^7.586*y + (t^7.724*y)/g1 + 2*g1^18*t^7.965*y + 2*g1^4*t^8.103*y + (t^8.242*y)/g1^10 - g1^23*t^8.344*y + 4*g1^9*t^8.483*y + (2*t^8.621*y)/g1^5 + 2*g1^14*t^8.862*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 |
|---|---|---|---|---|---|---|---|---|
| 46783 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ | 0.5615 | 0.7236 | 0.776 | [M:[0.6841, 1.1484, 0.9808, 0.7225], q:[0.2967, 1.0192], qb:[0.5549, 0.4258], phi:[0.4258]] | t^2.052 + 2*t^2.168 + t^2.555 + 2*t^2.942 + 2*t^3.445 + t^4.104 + 2*t^4.22 + 4*t^4.335 + t^4.607 + 3*t^4.723 + 2*t^4.994 + 4*t^5.11 + 3*t^5.497 + 3*t^5.613 + 3*t^5.885 - 2*t^6. - t^4.277/y - t^4.277*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46061 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$ | 0.5407 | 0.6833 | 0.7913 | [M:[0.7245, 1.141], q:[0.282, 0.9935], qb:[0.577, 0.4295], phi:[0.4295]] | t^2.134 + t^2.174 + t^2.577 + t^2.98 + t^3.02 + 2*t^3.423 + t^3.866 + 2*t^4.269 + t^4.308 + t^4.347 + 2*t^4.711 + t^4.751 + t^5.115 + 2*t^5.154 + t^5.193 + 2*t^5.557 + 2*t^5.597 + t^5.961 - t^4.289/y - t^4.289*y | detail |