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 |
|---|---|---|---|---|---|---|---|---|---|
| 4320 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{3}X_{1}$ + ${ }M_{8}\phi_{1}q_{1}^{2}$ | 0.6821 | 0.8675 | 0.7862 | [X:[1.5536], M:[0.8265, 1.2066, 0.4464, 0.7934, 0.8265, 0.8596, 0.7602, 0.8265], q:[0.3801, 0.7934], qb:[0.4133, 0.7602], phi:[0.4133]] | [X:[[7]], M:[[-4], [-1], [-7], [1], [-4], [-9], [6], [-4]], q:[[3], [1]], qb:[[-2], [6]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{7}$, ${ }M_{4}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{7}^{2}$, ${ }M_{4}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{7}M_{8}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{6}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{1}M_{8}$, ${ }M_{5}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{8}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{7}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$ | ${}M_{4}\phi_{1}q_{1}\tilde{q}_{1}$ | -2 | t^2.281 + t^2.38 + 4*t^2.48 + t^2.579 + 2*t^3.62 + t^4.561 + 3*t^4.661 + 6*t^4.76 + 4*t^4.86 + 10*t^4.959 + 4*t^5.058 + t^5.158 + t^5.801 + t^5.901 - 2*t^6. + 4*t^6.099 + t^6.199 + t^6.842 + 3*t^6.942 + 4*t^7.041 + 7*t^7.14 + 16*t^7.24 + 10*t^7.339 + 21*t^7.439 + 10*t^7.538 + 4*t^7.637 + t^7.737 + t^8.082 - t^8.181 - t^8.281 - 3*t^8.38 - 11*t^8.48 + 2*t^8.579 + t^8.778 - t^4.24/y - t^6.52/y - (4*t^6.719)/y - t^6.819/y + (2*t^7.661)/y + (8*t^7.76)/y + (5*t^7.86)/y + (8*t^7.959)/y + (4*t^8.058)/y - t^8.801/y + (2*t^8.901)/y - t^4.24*y - t^6.52*y - 4*t^6.719*y - t^6.819*y + 2*t^7.661*y + 8*t^7.76*y + 5*t^7.86*y + 8*t^7.959*y + 4*t^8.058*y - t^8.801*y + 2*t^8.901*y | g1^6*t^2.281 + g1*t^2.38 + (4*t^2.48)/g1^4 + t^2.579/g1^9 + (2*t^3.62)/g1 + g1^12*t^4.561 + 3*g1^7*t^4.661 + 6*g1^2*t^4.76 + (4*t^4.86)/g1^3 + (10*t^4.959)/g1^8 + (4*t^5.058)/g1^13 + t^5.158/g1^18 + g1^10*t^5.801 + g1^5*t^5.901 - 2*t^6. + (4*t^6.099)/g1^5 + t^6.199/g1^10 + g1^18*t^6.842 + 3*g1^13*t^6.942 + 4*g1^8*t^7.041 + 7*g1^3*t^7.14 + (16*t^7.24)/g1^2 + (10*t^7.339)/g1^7 + (21*t^7.439)/g1^12 + (10*t^7.538)/g1^17 + (4*t^7.637)/g1^22 + t^7.737/g1^27 + g1^16*t^8.082 - g1^11*t^8.181 - g1^6*t^8.281 - 3*g1*t^8.38 - (11*t^8.48)/g1^4 + (2*t^8.579)/g1^9 + t^8.778/g1^19 - t^4.24/(g1^2*y) - (g1^4*t^6.52)/y - (4*t^6.719)/(g1^6*y) - t^6.819/(g1^11*y) + (2*g1^7*t^7.661)/y + (8*g1^2*t^7.76)/y + (5*t^7.86)/(g1^3*y) + (8*t^7.959)/(g1^8*y) + (4*t^8.058)/(g1^13*y) - (g1^10*t^8.801)/y + (2*g1^5*t^8.901)/y - (t^4.24*y)/g1^2 - g1^4*t^6.52*y - (4*t^6.719*y)/g1^6 - (t^6.819*y)/g1^11 + 2*g1^7*t^7.661*y + 8*g1^2*t^7.76*y + (5*t^7.86*y)/g1^3 + (8*t^7.959*y)/g1^8 + (4*t^8.058*y)/g1^13 - g1^10*t^8.801*y + 2*g1^5*t^8.901*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2322 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{3}X_{1}$ | 0.6676 | 0.842 | 0.7928 | [X:[1.5364], M:[0.8363, 1.2091, 0.4636, 0.7909, 0.8363, 0.8818, 0.7455], q:[0.3727, 0.7909], qb:[0.4182, 0.7455], phi:[0.4182]] | t^2.236 + t^2.373 + 3*t^2.509 + t^2.645 + t^3.491 + 2*t^3.627 + t^4.473 + 3*t^4.609 + 5*t^4.745 + 3*t^4.882 + 6*t^5.018 + 3*t^5.154 + t^5.291 + 2*t^5.727 + 2*t^5.864 + t^6. - t^4.255/y - t^4.255*y | detail |