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 |
|---|---|---|---|---|---|---|---|---|---|
| 57379 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}X_{2}$ | 1.2142 | 1.4017 | 0.8662 | [X:[1.2851, 1.4297], M:[0.8595], q:[0.2142, 0.7845], qb:[0.5007, 0.3561], phi:[0.3574]] | [X:[[0, -2], [0, 4]], M:[[0, 8]], q:[[-1, -4], [-1, -8]], qb:[[1, 6], [1, 0]], phi:[[0, 1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }X_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ | ${}\phi_{1}^{4}q_{1}\tilde{q}_{2}$, ${ 2}\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}X_{1}$ | 2 | t^2.145 + t^2.578 + t^2.783 + 2*t^3.217 + 3*t^3.855 + 2*t^4.289 + t^4.494 + 2*t^4.711 + t^4.723 + 2*t^4.928 + 2*t^5.145 + t^5.157 + 2*t^5.362 + t^5.566 + 2*t^5.783 + 2*t^5.795 + 2*t^6. + 2*t^6.422 + 6*t^6.434 + 2*t^6.638 + 2*t^6.855 + 2*t^6.868 + 6*t^7.072 + t^7.277 + 2*t^7.289 + t^7.301 + 2*t^7.494 + 4*t^7.506 + 6*t^7.711 + 2*t^7.723 + t^7.735 + 2*t^7.928 + 2*t^7.94 + 5*t^8.145 + 3*t^8.349 + 4*t^8.362 + 2*t^8.374 + 4*t^8.566 + 4*t^8.578 + t^8.783 + t^8.988 - t^4.072/y - t^5.145/y - t^6.217/y - t^6.651/y - (2*t^7.289)/y - t^7.928/y + t^8.795/y - t^4.072*y - t^5.145*y - t^6.217*y - t^6.651*y - 2*t^7.289*y - t^7.928*y + t^8.795*y | g2^2*t^2.145 + g2^8*t^2.578 + t^2.783/g2^3 + 2*g2^3*t^3.217 + (3*t^3.855)/g2^2 + 2*g2^4*t^4.289 + t^4.494/g2^7 + t^4.711/(g1^3*g2^15) + g1^3*g2^7*t^4.711 + g2^10*t^4.723 + (2*t^4.928)/g2 + t^5.145/(g1^3*g2^9) + g1^3*g2^13*t^5.145 + g2^16*t^5.157 + 2*g2^5*t^5.362 + t^5.566/g2^6 + t^5.783/(g1^3*g2^14) + g1^3*g2^8*t^5.783 + 2*g2^11*t^5.795 + 2*t^6. + t^6.422/(g1^3*g2^19) + g1^3*g2^3*t^6.422 + 6*g2^6*t^6.434 + (2*t^6.638)/g2^5 + t^6.855/(g1^3*g2^13) + g1^3*g2^9*t^6.855 + 2*g2^12*t^6.868 + 6*g2*t^7.072 + t^7.277/g2^10 + t^7.289/(g1^3*g2^7) + g1^3*g2^15*t^7.289 + g2^18*t^7.301 + t^7.494/(g1^3*g2^18) + g1^3*g2^4*t^7.494 + 4*g2^7*t^7.506 + (6*t^7.711)/g2^4 + t^7.723/(g1^3*g2) + g1^3*g2^21*t^7.723 + g2^24*t^7.735 + t^7.928/(g1^3*g2^12) + g1^3*g2^10*t^7.928 + 2*g2^13*t^7.94 + 5*g2^2*t^8.145 + (3*t^8.349)/g2^9 + (2*t^8.362)/(g1^3*g2^6) + 2*g1^3*g2^16*t^8.362 + 2*g2^19*t^8.374 + (2*t^8.566)/(g1^3*g2^17) + 2*g1^3*g2^5*t^8.566 + 4*g2^8*t^8.578 + t^8.783/g2^3 + t^8.988/g2^14 - (g2*t^4.072)/y - (g2^2*t^5.145)/y - (g2^3*t^6.217)/y - (g2^9*t^6.651)/y - (2*g2^4*t^7.289)/y - t^7.928/(g2*y) + (g2^11*t^8.795)/y - g2*t^4.072*y - g2^2*t^5.145*y - g2^3*t^6.217*y - g2^9*t^6.651*y - 2*g2^4*t^7.289*y - (t^7.928*y)/g2 + g2^11*t^8.795*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47886 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.4552 | 1.6417 | 0.8864 | [X:[1.3445], M:[0.9482], q:[0.49, 0.5268], qb:[0.4916, 0.525], phi:[0.3278]] | t^2.845 + t^2.945 + t^2.95 + t^3.045 + t^3.055 + t^3.928 + t^4.028 + t^4.033 + t^4.038 + t^4.139 + t^4.911 + t^5.012 + t^5.022 + t^5.122 + t^5.504 + t^5.508 + t^5.608 + t^5.614 + t^5.689 + t^5.789 + t^5.794 + t^5.89 + t^5.895 + t^5.9 + t^5.99 + t^5.995 - 3*t^6. - t^3.983/y - t^4.967/y - t^3.983*y - t^4.967*y | detail |