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 |
|---|---|---|---|---|---|---|---|---|---|
| 55120 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6077 | 0.776 | 0.7831 | [M:[1.0, 0.9351, 0.7257, 1.2743, 1.0325, 0.7581], q:[0.7581, 0.2419], qb:[0.5162, 0.5487], phi:[0.4838]] | [M:[[0], [-8], [-3], [3], [4], [1]], q:[[1], [-1]], qb:[[2], [6]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }M_{1}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{2}q_{2}^{4}$ | ${}M_{5}\phi_{1}q_{2}^{2}$ | -2 | 2*t^2.274 + t^2.372 + t^2.805 + t^2.903 + t^3. + t^3.097 + 2*t^3.823 + t^3.92 + 4*t^4.549 + 3*t^4.646 + 2*t^4.743 + t^5.08 + 2*t^5.177 + 3*t^5.274 + 3*t^5.372 + t^5.469 + t^5.61 + t^5.708 + 2*t^5.805 - 2*t^6. + 3*t^6.097 + 4*t^6.195 + t^6.292 - t^6.531 + 5*t^6.823 + 6*t^6.92 + 5*t^7.018 + 2*t^7.115 + t^7.354 + t^7.451 + 3*t^7.549 + 8*t^7.646 + 5*t^7.743 + 2*t^7.841 + t^7.885 + t^7.982 + 3*t^8.08 - 6*t^8.274 + t^8.372 + t^8.416 + 6*t^8.469 + t^8.513 + 6*t^8.567 + 2*t^8.61 + 2*t^8.664 + 2*t^8.708 - 3*t^8.805 - 4*t^8.903 - t^4.451/y - t^6.726/y - t^7.257/y + t^7.549/y + (3*t^7.646)/y + (2*t^8.08)/y + (4*t^8.177)/y + (3*t^8.274)/y + (3*t^8.372)/y + t^8.469/y + t^8.708/y + t^8.805/y + (2*t^8.903)/y - t^4.451*y - t^6.726*y - t^7.257*y + t^7.549*y + 3*t^7.646*y + 2*t^8.08*y + 4*t^8.177*y + 3*t^8.274*y + 3*t^8.372*y + t^8.469*y + t^8.708*y + t^8.805*y + 2*t^8.903*y | 2*g1*t^2.274 + g1^5*t^2.372 + t^2.805/g1^8 + t^2.903/g1^4 + t^3. + g1^4*t^3.097 + 2*g1^3*t^3.823 + g1^7*t^3.92 + 4*g1^2*t^4.549 + 3*g1^6*t^4.646 + 2*g1^10*t^4.743 + t^5.08/g1^7 + (2*t^5.177)/g1^3 + 3*g1*t^5.274 + 3*g1^5*t^5.372 + g1^9*t^5.469 + t^5.61/g1^16 + t^5.708/g1^12 + (2*t^5.805)/g1^8 - 2*t^6. + 3*g1^4*t^6.097 + 4*g1^8*t^6.195 + g1^12*t^6.292 - t^6.531/g1^9 + 5*g1^3*t^6.823 + 6*g1^7*t^6.92 + 5*g1^11*t^7.018 + 2*g1^15*t^7.115 + t^7.354/g1^6 + t^7.451/g1^2 + 3*g1^2*t^7.549 + 8*g1^6*t^7.646 + 5*g1^10*t^7.743 + 2*g1^14*t^7.841 + t^7.885/g1^15 + t^7.982/g1^11 + (3*t^8.08)/g1^7 - 6*g1*t^8.274 + g1^5*t^8.372 + t^8.416/g1^24 + 6*g1^9*t^8.469 + t^8.513/g1^20 + 6*g1^13*t^8.567 + (2*t^8.61)/g1^16 + 2*g1^17*t^8.664 + (2*t^8.708)/g1^12 - (3*t^8.805)/g1^8 - (4*t^8.903)/g1^4 - t^4.451/(g1^2*y) - t^6.726/(g1*y) - t^7.257/(g1^10*y) + (g1^2*t^7.549)/y + (3*g1^6*t^7.646)/y + (2*t^8.08)/(g1^7*y) + (4*t^8.177)/(g1^3*y) + (3*g1*t^8.274)/y + (3*g1^5*t^8.372)/y + (g1^9*t^8.469)/y + t^8.708/(g1^12*y) + t^8.805/(g1^8*y) + (2*t^8.903)/(g1^4*y) - (t^4.451*y)/g1^2 - (t^6.726*y)/g1 - (t^7.257*y)/g1^10 + g1^2*t^7.549*y + 3*g1^6*t^7.646*y + (2*t^8.08*y)/g1^7 + (4*t^8.177*y)/g1^3 + 3*g1*t^8.274*y + 3*g1^5*t^8.372*y + g1^9*t^8.469*y + (t^8.708*y)/g1^12 + (t^8.805*y)/g1^8 + (2*t^8.903*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46866 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{5}\phi_{1}^{2}$ | 0.589 | 0.742 | 0.7938 | [M:[1.0, 0.9307, 0.724, 1.276, 1.0346], q:[0.7587, 0.2413], qb:[0.5173, 0.552], phi:[0.4827]] | t^2.276 + t^2.38 + t^2.792 + t^2.896 + t^3. + t^3.104 + t^3.724 + 2*t^3.828 + t^3.932 + 2*t^4.552 + 2*t^4.656 + 2*t^4.76 + t^5.172 + 2*t^5.276 + 2*t^5.38 + t^5.484 + t^5.584 + t^5.688 + 2*t^5.792 - t^6. - t^4.448/y - t^4.448*y | detail |