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 |
|---|---|---|---|---|---|---|---|---|---|
| 53834 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ | 0.7172 | 0.8838 | 0.8115 | [M:[0.8014, 0.9338, 1.0662, 0.9338, 1.0, 0.9338], q:[0.5662, 0.6324], qb:[0.5, 0.4338], phi:[0.4669]] | [M:[[6], [2], [-2], [2], [0], [2]], q:[[-2], [-4]], qb:[[0], [2]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{2}$, ${ }M_{4}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{5}\phi_{1}^{2}$ | ${}$ | -3 | t^2.404 + 4*t^2.801 + t^3. + t^3.397 + t^4.003 + t^4.202 + 2*t^4.401 + 2*t^4.599 + 2*t^4.798 + t^4.808 + t^4.997 + t^5.195 + 4*t^5.206 + 8*t^5.603 + 2*t^5.801 - 3*t^6. + t^6.199 - 2*t^6.397 + t^6.408 - t^6.596 + t^6.606 + t^6.794 + 5*t^6.805 + 5*t^7.003 + 6*t^7.202 + t^7.212 + 6*t^7.401 + 4*t^7.599 + 4*t^7.61 + t^7.798 + t^7.997 + 9*t^8.007 - t^8.394 + 11*t^8.404 + t^8.592 + 3*t^8.603 - 11*t^8.801 + t^8.812 - t^4.401/y - t^6.805/y - (3*t^7.202)/y + (3*t^7.599)/y + t^7.997/y + (4*t^8.206)/y + t^8.404/y + (6*t^8.603)/y + (5*t^8.801)/y - t^4.401*y - t^6.805*y - 3*t^7.202*y + 3*t^7.599*y + t^7.997*y + 4*t^8.206*y + t^8.404*y + 6*t^8.603*y + 5*t^8.801*y | g1^6*t^2.404 + 4*g1^2*t^2.801 + t^3. + t^3.397/g1^4 + g1^5*t^4.003 + g1^3*t^4.202 + 2*g1*t^4.401 + (2*t^4.599)/g1 + (2*t^4.798)/g1^3 + g1^12*t^4.808 + t^4.997/g1^5 + t^5.195/g1^7 + 4*g1^8*t^5.206 + 8*g1^4*t^5.603 + 2*g1^2*t^5.801 - 3*t^6. + t^6.199/g1^2 - (2*t^6.397)/g1^4 + g1^11*t^6.408 - t^6.596/g1^6 + g1^9*t^6.606 + t^6.794/g1^8 + 5*g1^7*t^6.805 + 5*g1^5*t^7.003 + 6*g1^3*t^7.202 + g1^18*t^7.212 + 6*g1*t^7.401 + (4*t^7.599)/g1 + 4*g1^14*t^7.61 + t^7.798/g1^3 + t^7.997/g1^5 + 9*g1^10*t^8.007 - t^8.394/g1^9 + 11*g1^6*t^8.404 + t^8.592/g1^11 + 3*g1^4*t^8.603 - 11*g1^2*t^8.801 + g1^17*t^8.812 - (g1*t^4.401)/y - (g1^7*t^6.805)/y - (3*g1^3*t^7.202)/y + (3*t^7.599)/(g1*y) + t^7.997/(g1^5*y) + (4*g1^8*t^8.206)/y + (g1^6*t^8.404)/y + (6*g1^4*t^8.603)/y + (5*g1^2*t^8.801)/y - g1*t^4.401*y - g1^7*t^6.805*y - 3*g1^3*t^7.202*y + (3*t^7.599*y)/g1 + (t^7.997*y)/g1^5 + 4*g1^8*t^8.206*y + g1^6*t^8.404*y + 6*g1^4*t^8.603*y + 5*g1^2*t^8.801*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 |
|---|---|---|---|---|---|---|---|---|
| 56494 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{7}q_{2}\tilde{q}_{1}$ | 0.7299 | 0.9081 | 0.8038 | [M:[0.7659, 0.922, 1.078, 0.922, 1.0, 0.922, 0.8439], q:[0.578, 0.6561], qb:[0.5, 0.422], phi:[0.461]] | t^2.298 + t^2.532 + 4*t^2.766 + t^3. + t^3.915 + t^4.149 + 2*t^4.383 + t^4.595 + 2*t^4.617 + t^4.83 + 2*t^4.851 + 5*t^5.064 + t^5.085 + 4*t^5.298 + t^5.319 + 9*t^5.532 + t^5.766 - 3*t^6. - t^4.383/y - t^4.383*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47096 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}\phi_{1}^{2}$ | 0.7114 | 0.8731 | 0.8147 | [M:[0.8238, 0.9413, 1.0587, 0.9413, 1.0], q:[0.5587, 0.6175], qb:[0.5, 0.4413], phi:[0.4706]] | t^2.471 + 3*t^2.824 + t^3. + t^3.176 + t^3.352 + t^4.059 + t^4.236 + 2*t^4.412 + 2*t^4.588 + 2*t^4.764 + t^4.941 + t^4.943 + t^5.117 + 3*t^5.295 + 5*t^5.648 + t^5.824 - t^4.412/y - t^4.412*y | detail |