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 |
|---|---|---|---|---|---|---|---|---|---|
| 6464 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{3}M_{7}$ + ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{8}^{2}$ + ${ }M_{6}X_{1}$ | 0.6091 | 0.7631 | 0.7982 | [X:[1.4286], M:[0.8929, 0.9643, 1.1071, 0.75, 1.25, 0.5714, 0.8929, 1.0], q:[0.625, 0.4821], qb:[0.2679, 0.7679], phi:[0.4643]] | [X:[[0]], M:[[0], [0], [0], [0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 427887/702464, c: 536079/702464, X1: 10/7, M1: 25/28, M2: 27/28, M3: 31/28, M4: 3/4, M5: 5/4, M6: 4/7, M7: 25/28, M8: 1, q1: 5/8, q2: 27/56, qb1: 15/56, qb2: 43/56, phi1: 13/28} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{1}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{8}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}M_{8}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{7}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{2}M_{8}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ | ${}$ | -1 | t^2.25 + 2*t^2.679 + t^2.786 + t^2.893 + t^3. + t^3.643 + t^3.75 + t^4.071 + t^4.179 + t^4.286 + t^4.5 + t^4.714 + t^4.929 + t^5.036 + 2*t^5.143 + t^5.25 + 2*t^5.357 + 2*t^5.464 + 2*t^5.571 + 3*t^5.679 + 2*t^5.786 + t^5.893 - t^6. - t^6.214 + t^6.321 + t^6.429 + 2*t^6.536 + t^6.643 + 2*t^6.75 + t^6.857 + 2*t^6.964 + 2*t^7.071 + 2*t^7.179 + t^7.286 + t^7.393 + t^7.5 + t^7.607 + t^7.714 + 2*t^7.821 + 4*t^7.929 + 5*t^8.036 + 4*t^8.143 + 2*t^8.25 + 4*t^8.357 + 3*t^8.464 + 3*t^8.571 - t^8.679 - 3*t^8.893 - t^4.393/y - t^7.071/y - t^7.179/y - t^7.286/y + t^7.5/y + t^7.607/y + t^7.714/y + (2*t^7.929)/y + t^8.036/y + t^8.143/y + t^8.25/y + t^8.357/y + (2*t^8.464)/y + (2*t^8.571)/y + (3*t^8.679)/y + t^8.786/y + (2*t^8.893)/y - t^4.393*y - t^7.071*y - t^7.179*y - t^7.286*y + t^7.5*y + t^7.607*y + t^7.714*y + 2*t^7.929*y + t^8.036*y + t^8.143*y + t^8.25*y + t^8.357*y + 2*t^8.464*y + 2*t^8.571*y + 3*t^8.679*y + t^8.786*y + 2*t^8.893*y | t^2.25 + 2*t^2.679 + t^2.786 + t^2.893 + t^3. + t^3.643 + t^3.75 + t^4.071 + t^4.179 + t^4.286 + t^4.5 + t^4.714 + t^4.929 + t^5.036 + 2*t^5.143 + t^5.25 + 2*t^5.357 + 2*t^5.464 + 2*t^5.571 + 3*t^5.679 + 2*t^5.786 + t^5.893 - t^6. - t^6.214 + t^6.321 + t^6.429 + 2*t^6.536 + t^6.643 + 2*t^6.75 + t^6.857 + 2*t^6.964 + 2*t^7.071 + 2*t^7.179 + t^7.286 + t^7.393 + t^7.5 + t^7.607 + t^7.714 + 2*t^7.821 + 4*t^7.929 + 5*t^8.036 + 4*t^8.143 + 2*t^8.25 + 4*t^8.357 + 3*t^8.464 + 3*t^8.571 - t^8.679 - 3*t^8.893 - t^4.393/y - t^7.071/y - t^7.179/y - t^7.286/y + t^7.5/y + t^7.607/y + t^7.714/y + (2*t^7.929)/y + t^8.036/y + t^8.143/y + t^8.25/y + t^8.357/y + (2*t^8.464)/y + (2*t^8.571)/y + (3*t^8.679)/y + t^8.786/y + (2*t^8.893)/y - t^4.393*y - t^7.071*y - t^7.179*y - t^7.286*y + t^7.5*y + t^7.607*y + t^7.714*y + 2*t^7.929*y + t^8.036*y + t^8.143*y + t^8.25*y + t^8.357*y + 2*t^8.464*y + 2*t^8.571*y + 3*t^8.679*y + t^8.786*y + 2*t^8.893*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 4831 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{3}M_{7}$ + ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$ | 0.7001 | 0.889 | 0.7875 | [M:[1.0224, 0.7877, 0.9776, 0.8324, 1.1676, 0.7598, 1.0224, 0.6703], q:[0.5838, 0.3938], qb:[0.4386, 0.7737], phi:[0.4525]] | t^2.011 + t^2.279 + t^2.363 + t^2.497 + t^2.715 + 2*t^3.067 + t^3.503 + t^3.855 + t^4.022 + t^4.073 + 2*t^4.29 + t^4.374 + t^4.425 + t^4.508 + t^4.559 + t^4.642 + 2*t^4.726 + t^4.777 + 2*t^4.86 + 2*t^4.995 + 3*t^5.078 + t^5.212 + 2*t^5.347 + 2*t^5.43 + t^5.514 + t^5.564 + 3*t^5.782 + t^5.866 - 2*t^6. - t^4.358/y - t^4.358*y | detail |