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 |
|---|---|---|---|---|---|---|---|---|---|
| 58264 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{7}\phi_{1}^{2}$ + ${ }M_{8}\phi_{1}q_{1}q_{2}$ | 0.6262 | 0.7767 | 0.8062 | [X:[1.4088], M:[1.0912, 1.0438, 0.9088, 0.5912, 1.0, 0.7263, 1.1825, 0.6825], q:[0.2956, 0.6131], qb:[0.6606, 0.7956], phi:[0.4088]] | [X:[[2]], M:[[-2], [10], [2], [-2], [0], [6], [-4], [-4]], q:[[-1], [3]], qb:[[-9], [-1]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{8}$, ${ }M_{6}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{2}$, ${ }M_{1}$, ${ }M_{7}$, ${ }M_{8}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{6}M_{8}$, ${ }X_{1}$, ${ }M_{6}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{8}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}M_{8}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{8}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{1}M_{8}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{6}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{7}M_{8}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{6}M_{7}$ | ${}$ | -1 | t^2.047 + t^2.179 + t^2.726 + t^3. + t^3.131 + t^3.274 + t^3.547 + 2*t^4.095 + 2*t^4.226 + t^4.358 + t^4.369 + t^4.774 + t^4.905 + t^5.047 + 2*t^5.179 + t^5.19 + t^5.31 + t^5.321 + 2*t^5.453 + t^5.595 + t^5.726 - t^6. + t^6.142 + t^6.263 + 4*t^6.274 + 2*t^6.405 + t^6.416 + t^6.537 + t^6.547 + t^6.821 + t^6.953 + 2*t^7.095 + t^7.226 + t^7.237 + 3*t^7.358 + 2*t^7.369 + t^7.489 + 2*t^7.5 + 2*t^7.631 + 2*t^7.642 + t^7.774 + t^7.916 + t^8.037 - 3*t^8.047 - t^8.179 + 2*t^8.19 + t^8.31 + 3*t^8.321 + t^8.442 + 4*t^8.453 + 2*t^8.463 + 2*t^8.584 + t^8.595 + t^8.715 - t^8.726 + t^8.737 - t^4.226/y - t^6.274/y - t^6.405/y + t^7.095/y + t^7.226/y - t^7.358/y + t^7.774/y + t^7.905/y + (2*t^8.047)/y + (3*t^8.179)/y + t^8.31/y - t^8.584/y + t^8.595/y + (2*t^8.726)/y + t^8.858/y - t^4.226*y - t^6.274*y - t^6.405*y + t^7.095*y + t^7.226*y - t^7.358*y + t^7.774*y + t^7.905*y + 2*t^8.047*y + 3*t^8.179*y + t^8.31*y - t^8.584*y + t^8.595*y + 2*t^8.726*y + t^8.858*y | t^2.047/g1^4 + g1^6*t^2.179 + g1^2*t^2.726 + t^3. + g1^10*t^3.131 + t^3.274/g1^2 + t^3.547/g1^4 + (2*t^4.095)/g1^8 + 2*g1^2*t^4.226 + g1^12*t^4.358 + t^4.369/g1^10 + t^4.774/g1^2 + g1^8*t^4.905 + t^5.047/g1^4 + 2*g1^6*t^5.179 + t^5.19/g1^16 + g1^16*t^5.31 + t^5.321/g1^6 + 2*g1^4*t^5.453 + t^5.595/g1^8 + g1^2*t^5.726 - t^6. + t^6.142/g1^12 + g1^20*t^6.263 + (4*t^6.274)/g1^2 + 2*g1^8*t^6.405 + t^6.416/g1^14 + g1^18*t^6.537 + t^6.547/g1^4 + t^6.821/g1^6 + g1^4*t^6.953 + (2*t^7.095)/g1^8 + g1^2*t^7.226 + t^7.237/g1^20 + 3*g1^12*t^7.358 + (2*t^7.369)/g1^10 + g1^22*t^7.489 + 2*t^7.5 + 2*g1^10*t^7.631 + (2*t^7.642)/g1^12 + t^7.774/g1^2 + t^7.916/g1^14 + g1^18*t^8.037 - (3*t^8.047)/g1^4 - g1^6*t^8.179 + (2*t^8.19)/g1^16 + g1^16*t^8.31 + (3*t^8.321)/g1^6 + g1^26*t^8.442 + 4*g1^4*t^8.453 + (2*t^8.463)/g1^18 + 2*g1^14*t^8.584 + t^8.595/g1^8 + g1^24*t^8.715 - g1^2*t^8.726 + t^8.737/g1^20 - (g1^2*t^4.226)/y - t^6.274/(g1^2*y) - (g1^8*t^6.405)/y + t^7.095/(g1^8*y) + (g1^2*t^7.226)/y - (g1^12*t^7.358)/y + t^7.774/(g1^2*y) + (g1^8*t^7.905)/y + (2*t^8.047)/(g1^4*y) + (3*g1^6*t^8.179)/y + (g1^16*t^8.31)/y - (g1^14*t^8.584)/y + t^8.595/(g1^8*y) + (2*g1^2*t^8.726)/y + (g1^12*t^8.858)/y - g1^2*t^4.226*y - (t^6.274*y)/g1^2 - g1^8*t^6.405*y + (t^7.095*y)/g1^8 + g1^2*t^7.226*y - g1^12*t^7.358*y + (t^7.774*y)/g1^2 + g1^8*t^7.905*y + (2*t^8.047*y)/g1^4 + 3*g1^6*t^8.179*y + g1^16*t^8.31*y - g1^14*t^8.584*y + (t^8.595*y)/g1^8 + 2*g1^2*t^8.726*y + g1^12*t^8.858*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 |
|---|---|---|---|---|---|---|---|---|---|
| 56109 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6054 | 0.7362 | 0.8224 | [X:[1.4082], M:[1.0918, 1.041, 0.9082, 0.5918, 1.0, 0.7246, 1.1836], q:[0.2959, 0.6123], qb:[0.6631, 0.7959], phi:[0.4082]] | t^2.174 + t^2.725 + t^3. + t^3.123 + t^3.275 + t^3.551 + t^3.949 + t^4.102 + t^4.225 + t^4.348 + t^4.377 + t^4.898 + t^5.174 + t^5.203 + t^5.297 + 2*t^5.449 + t^5.725 - t^6. - t^4.225/y - t^4.225*y | detail |