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 |
|---|---|---|---|---|---|---|---|---|---|
| 54907 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{2}^{2}$ | 0.5738 | 0.7167 | 0.8007 | [X:[1.5714], M:[0.4286, 1.0, 1.2857, 0.7143, 1.1429, 0.7143], q:[0.6786, 0.8929], qb:[0.3214, 0.3929], phi:[0.4286]] | [X:[[0]], M:[[0], [0], [0], [0], [0], [0]], q:[[1], [-1]], qb:[[-1], [1]], phi:[[0]]] | 1 | {a: 12597/21952, c: 15733/21952, X1: 11/7, M1: 3/7, M2: 1, M3: 9/7, M4: 5/7, M5: 8/7, M6: 5/7, q1: 19/28, q2: 25/28, qb1: 9/28, qb2: 11/28, phi1: 3/7} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{6}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$ | ${}$ | -2 | 2*t^2.143 + t^3. + 2*t^3.214 + 2*t^3.429 + 2*t^3.643 + 3*t^4.286 + t^4.714 + 2*t^5.143 + 4*t^5.357 + 3*t^5.571 + 2*t^5.786 - 2*t^6. + 7*t^6.429 + 4*t^6.643 + 5*t^6.857 + 3*t^7.286 + 4*t^7.5 + 3*t^7.714 + 2*t^7.929 - 4*t^8.143 + 10*t^8.571 + 4*t^8.786 - t^4.286/y - t^6.429/y + t^7.286/y + (3*t^8.143)/y + (4*t^8.357)/y + (3*t^8.571)/y + (4*t^8.786)/y - t^4.286*y - t^6.429*y + t^7.286*y + 3*t^8.143*y + 4*t^8.357*y + 3*t^8.571*y + 4*t^8.786*y | 2*t^2.143 + t^3. + t^3.214/g1^2 + g1^2*t^3.214 + 2*t^3.429 + t^3.643/g1^2 + g1^2*t^3.643 + 3*t^4.286 + t^4.714 + 2*t^5.143 + (2*t^5.357)/g1^2 + 2*g1^2*t^5.357 + 3*t^5.571 + t^5.786/g1^2 + g1^2*t^5.786 - 2*t^6. + 5*t^6.429 + t^6.429/g1^4 + g1^4*t^6.429 + (2*t^6.643)/g1^2 + 2*g1^2*t^6.643 + 3*t^6.857 + t^6.857/g1^4 + g1^4*t^6.857 + t^7.286 + t^7.286/g1^4 + g1^4*t^7.286 + (2*t^7.5)/g1^2 + 2*g1^2*t^7.5 + 3*t^7.714 + t^7.929/g1^2 + g1^2*t^7.929 - 4*t^8.143 + 6*t^8.571 + (2*t^8.571)/g1^4 + 2*g1^4*t^8.571 + (2*t^8.786)/g1^2 + 2*g1^2*t^8.786 - t^4.286/y - t^6.429/y + t^7.286/y + (3*t^8.143)/y + (2*t^8.357)/(g1^2*y) + (2*g1^2*t^8.357)/y + (3*t^8.571)/y + (2*t^8.786)/(g1^2*y) + (2*g1^2*t^8.786)/y - t^4.286*y - t^6.429*y + t^7.286*y + 3*t^8.143*y + (2*t^8.357*y)/g1^2 + 2*g1^2*t^8.357*y + 3*t^8.571*y + (2*t^8.786*y)/g1^2 + 2*g1^2*t^8.786*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 |
|---|---|---|---|---|---|---|---|---|
| 56626 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{2}^{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ | 0.5829 | 0.7337 | 0.7945 | [X:[1.5714], M:[0.4286, 1.0, 1.2857, 0.7143, 1.1429, 0.7143, 0.8731], q:[0.6509, 0.9206], qb:[0.3491, 0.3651], phi:[0.4286]] | 2*t^2.143 + t^2.619 + t^3. + t^3.048 + 2*t^3.429 + t^3.477 + t^3.809 + 3*t^4.286 + t^4.714 + 2*t^4.762 + 2*t^5.143 + 2*t^5.191 + t^5.239 + 3*t^5.571 + 2*t^5.619 + t^5.667 + t^5.952 - 2*t^6. - t^4.286/y - t^4.286*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46882 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ | 0.617 | 0.7524 | 0.82 | [X:[1.6109], M:[0.3891, 0.7236, 1.1673, 0.8327, 1.2218, 0.8327], q:[0.8464, 0.7645], qb:[0.43, 0.4027], phi:[0.3891]] | t^2.171 + 2*t^2.498 + 2*t^3.584 + 2*t^3.665 + 2*t^3.747 + t^4.342 + 2*t^4.669 + t^4.833 + 3*t^4.996 + 2*t^5.754 + t^5.836 - 3*t^6. - t^4.167/y - t^4.167*y | detail |