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 |
|---|---|---|---|---|---|---|---|---|---|
| 58274 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{2}M_{7}$ + ${ }M_{3}M_{8}$ | 0.6189 | 0.7601 | 0.8142 | [X:[1.4201], M:[1.0799, 1.1003, 0.9201, 0.5799, 1.0, 0.7602, 0.8997, 1.0799], q:[0.29, 0.6301], qb:[0.6097, 0.79], phi:[0.4201]] | [X:[[2]], M:[[-2], [10], [2], [-2], [0], [6], [-10], [-2]], q:[[-1], [3]], qb:[[-9], [-1]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{7}$, ${ }M_{5}$, ${ }M_{1}$, ${ }M_{8}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{7}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{8}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{7}M_{8}$ | ${}$ | -2 | t^2.281 + t^2.52 + t^2.699 + t^3. + 2*t^3.24 + t^3.959 + t^4.02 + t^4.199 + t^4.26 + t^4.561 + t^4.801 + t^4.919 + t^4.98 + t^5.041 + t^5.219 + t^5.281 + t^5.398 + 3*t^5.52 + t^5.699 + t^5.76 + t^5.939 - 2*t^6. - t^6.061 + 2*t^6.24 + 3*t^6.48 + t^6.541 + t^6.658 + t^6.842 + t^6.898 + t^7.081 + 2*t^7.199 + t^7.26 + 2*t^7.439 + t^7.5 + 2*t^7.561 + t^7.618 + 3*t^7.801 + 2*t^7.919 + 2*t^8.041 + t^8.097 + 2*t^8.158 + 2*t^8.219 - t^8.281 + t^8.398 - t^8.581 + t^8.638 - 2*t^8.699 + 2*t^8.76 + t^8.878 + t^8.939 - t^4.26/y - t^6.541/y - t^6.781/y + t^7.02/y - t^7.5/y + t^7.74/y + t^7.801/y + (2*t^7.98)/y + t^8.219/y + t^8.281/y + (3*t^8.52)/y + t^8.699/y + (2*t^8.76)/y - t^8.821/y + (2*t^8.939)/y - t^4.26*y - t^6.541*y - t^6.781*y + t^7.02*y - t^7.5*y + t^7.74*y + t^7.801*y + 2*t^7.98*y + t^8.219*y + t^8.281*y + 3*t^8.52*y + t^8.699*y + 2*t^8.76*y - t^8.821*y + 2*t^8.939*y | g1^6*t^2.281 + g1^4*t^2.52 + t^2.699/g1^10 + t^3. + (2*t^3.24)/g1^2 + t^3.959/g1^8 + g1^4*t^4.02 + t^4.199/g1^10 + g1^2*t^4.26 + g1^12*t^4.561 + g1^10*t^4.801 + t^4.919/g1^16 + t^4.98/g1^4 + g1^8*t^5.041 + t^5.219/g1^6 + g1^6*t^5.281 + t^5.398/g1^20 + 3*g1^4*t^5.52 + t^5.699/g1^10 + g1^2*t^5.76 + t^5.939/g1^12 - 2*t^6. - g1^12*t^6.061 + (2*t^6.24)/g1^2 + (3*t^6.48)/g1^4 + g1^8*t^6.541 + t^6.658/g1^18 + g1^18*t^6.842 + t^6.898/g1^20 + g1^16*t^7.081 + (2*t^7.199)/g1^10 + g1^2*t^7.26 + (2*t^7.439)/g1^12 + t^7.5 + 2*g1^12*t^7.561 + t^7.618/g1^26 + 3*g1^10*t^7.801 + (2*t^7.919)/g1^16 + 2*g1^8*t^8.041 + t^8.097/g1^30 + (2*t^8.158)/g1^18 + (2*t^8.219)/g1^6 - g1^6*t^8.281 + t^8.398/g1^20 - g1^16*t^8.581 + t^8.638/g1^22 - (2*t^8.699)/g1^10 + 2*g1^2*t^8.76 + t^8.878/g1^24 + t^8.939/g1^12 - (g1^2*t^4.26)/y - (g1^8*t^6.541)/y - (g1^6*t^6.781)/y + (g1^4*t^7.02)/y - t^7.5/y + t^7.74/(g1^2*y) + (g1^10*t^7.801)/y + (2*t^7.98)/(g1^4*y) + t^8.219/(g1^6*y) + (g1^6*t^8.281)/y + (3*g1^4*t^8.52)/y + t^8.699/(g1^10*y) + (2*g1^2*t^8.76)/y - (g1^14*t^8.821)/y + (2*t^8.939)/(g1^12*y) - g1^2*t^4.26*y - g1^8*t^6.541*y - g1^6*t^6.781*y + g1^4*t^7.02*y - t^7.5*y + (t^7.74*y)/g1^2 + g1^10*t^7.801*y + (2*t^7.98*y)/g1^4 + (t^8.219*y)/g1^6 + g1^6*t^8.281*y + 3*g1^4*t^8.52*y + (t^8.699*y)/g1^10 + 2*g1^2*t^8.76*y - g1^14*t^8.821*y + (2*t^8.939*y)/g1^12 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 56111 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{2}M_{7}$ | 0.6263 | 0.7723 | 0.811 | [X:[1.4176], M:[1.0824, 1.0882, 0.9176, 0.5824, 1.0, 0.7529, 0.9118], q:[0.2912, 0.6265], qb:[0.6206, 0.7912], phi:[0.4176]] | t^2.259 + t^2.506 + t^2.735 + t^2.753 + t^3. + t^3.247 + t^3.988 + t^4.006 + t^4.235 + t^4.253 + t^4.518 + t^4.765 + t^4.977 + t^4.994 + 2*t^5.012 + t^5.241 + 2*t^5.259 + t^5.471 + t^5.488 + 3*t^5.506 + t^5.735 + t^5.753 - t^6. - t^4.253/y - t^4.253*y | detail |