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 |
|---|---|---|---|---|---|---|---|---|---|
| 46266 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | 0.6133 | 0.7914 | 0.7749 | [M:[0.9637, 0.7409, 1.0363], q:[0.7409, 0.2954], qb:[0.4455, 0.4455], phi:[0.5182]] | [M:[[4], [1], [-4]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ | ${}$ | -2 | 3*t^2.223 + t^2.673 + 2*t^3.109 + t^3.327 + 2*t^3.559 + t^3.777 + 3*t^4.228 + 6*t^4.446 + 3*t^4.896 + 6*t^5.332 + t^5.346 + t^5.55 + 7*t^5.782 - 2*t^6. + t^6.218 + 2*t^6.233 + 2*t^6.436 + 6*t^6.45 + t^6.654 + 10*t^6.668 + 3*t^6.901 - t^7.104 + 6*t^7.119 + 3*t^7.337 + 8*t^7.554 + 3*t^7.569 + 4*t^7.787 + 12*t^8.005 + t^8.019 - 11*t^8.223 + 3*t^8.441 + 12*t^8.455 + 2*t^8.659 + 4*t^8.673 + t^8.876 + 15*t^8.891 + 2*t^8.906 - t^4.554/y - t^6.777/y + (4*t^7.446)/y - t^7.663/y + (3*t^7.896)/y + (7*t^8.332)/y + (3*t^8.55)/y + (8*t^8.782)/y - t^4.554*y - t^6.777*y + 4*t^7.446*y - t^7.663*y + 3*t^7.896*y + 7*t^8.332*y + 3*t^8.55*y + 8*t^8.782*y | 3*g1*t^2.223 + g1^12*t^2.673 + (2*t^3.109)/g1^4 + t^3.327/g1^12 + 2*g1^7*t^3.559 + t^3.777/g1 + 3*g1^10*t^4.228 + 6*g1^2*t^4.446 + 3*g1^13*t^4.896 + (6*t^5.332)/g1^3 + g1^24*t^5.346 + t^5.55/g1^11 + 7*g1^8*t^5.782 - 2*t^6. + t^6.218/g1^8 + 2*g1^19*t^6.233 + (2*t^6.436)/g1^16 + 6*g1^11*t^6.45 + t^6.654/g1^24 + 10*g1^3*t^6.668 + 3*g1^22*t^6.901 - t^7.104/g1^13 + 6*g1^14*t^7.119 + 3*g1^6*t^7.337 + (8*t^7.554)/g1^2 + 3*g1^25*t^7.569 + 4*g1^17*t^7.787 + 12*g1^9*t^8.005 + g1^36*t^8.019 - 11*g1*t^8.223 + (3*t^8.441)/g1^7 + 12*g1^20*t^8.455 + (2*t^8.659)/g1^15 + 4*g1^12*t^8.673 + t^8.876/g1^23 + 15*g1^4*t^8.891 + 2*g1^31*t^8.906 - t^4.554/(g1^2*y) - t^6.777/(g1*y) + (4*g1^2*t^7.446)/y - t^7.663/(g1^6*y) + (3*g1^13*t^7.896)/y + (7*t^8.332)/(g1^3*y) + (3*t^8.55)/(g1^11*y) + (8*g1^8*t^8.782)/y - (t^4.554*y)/g1^2 - (t^6.777*y)/g1 + 4*g1^2*t^7.446*y - (t^7.663*y)/g1^6 + 3*g1^13*t^7.896*y + (7*t^8.332*y)/g1^3 + (3*t^8.55*y)/g1^11 + 8*g1^8*t^8.782*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 |
|---|---|---|---|---|---|---|---|---|
| 46724 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6062 | 0.7779 | 0.7793 | [M:[0.9855, 0.7464, 1.0145, 1.0434], q:[0.7464, 0.2681], qb:[0.4783, 0.4783], phi:[0.5072]] | 3*t^2.239 + 2*t^3.043 + 2*t^3.13 + 2*t^3.674 + t^3.761 + 3*t^4.391 + 6*t^4.478 + 6*t^5.283 + 4*t^5.369 + 5*t^5.913 - 3*t^6. - t^4.522/y - t^4.522*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 |
|---|---|---|---|---|---|---|---|---|---|
| 45959 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{3}$ | 0.6135 | 0.7921 | 0.7745 | [M:[0.9638, 0.7321, 1.0362], q:[0.7409, 0.2953], qb:[0.4546, 0.4368], phi:[0.5181]] | 2*t^2.196 + t^2.249 + t^2.674 + 2*t^3.109 + t^3.326 + t^3.533 + t^3.587 + t^3.751 + t^4.175 + t^4.228 + t^4.282 + 3*t^4.392 + 2*t^4.446 + t^4.499 + 2*t^4.87 + t^4.924 + 4*t^5.305 + t^5.348 + 2*t^5.358 + t^5.522 + 2*t^5.73 + 4*t^5.783 + t^5.836 + t^5.947 - 2*t^6. - t^4.554/y - t^4.554*y | detail |