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 |
|---|---|---|---|---|---|---|---|---|---|
| 60486 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.4095 | 1.5959 | 0.8832 | [X:[1.372], M:[0.785], q:[0.5097, 0.4107], qb:[0.4903, 0.7053], phi:[0.314]] | [X:[[4]], M:[[-5]], q:[[1], [8]], qb:[[-1], [4]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{6}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ | ${}$ | -1 | t^2.35 + t^2.7 + t^2.83 + t^3. + t^3.35 + t^3.65 + t^3.94 + t^4.12 + t^4.29 + 2*t^4.59 + t^4.71 + t^4.88 + t^4.94 + t^5.06 + t^5.18 + 2*t^5.23 + t^5.41 + 2*t^5.53 + t^5.65 + t^5.7 + t^5.83 + t^5.88 - t^6. + t^6.05 + 2*t^6.17 - t^6.3 + 2*t^6.35 + 2*t^6.47 + t^6.52 + t^6.65 + t^6.7 + t^6.77 + 2*t^6.82 + 2*t^6.94 + 2*t^6.99 + t^7.06 + 3*t^7.12 + 4*t^7.29 + 4*t^7.41 + t^7.46 + t^7.54 + 3*t^7.59 + 2*t^7.64 + t^7.71 + 2*t^7.76 + 2*t^7.88 + 5*t^7.94 + t^8.01 + t^8.06 + t^8.11 - t^8.18 + 6*t^8.23 + t^8.28 - t^8.35 + t^8.41 + t^8.48 + 3*t^8.53 + 5*t^8.58 - t^8.7 + t^8.75 + t^8.83 + 8*t^8.88 + t^8.83/y^2 - t^3.94/y - t^4.88/y - t^6.3/y - t^6.65/y - t^6.77/y - t^6.94/y - t^7.24/y - t^7.29/y - t^7.59/y - t^7.71/y - t^7.88/y + t^8.06/y + t^8.18/y - t^8.23/y + t^8.35/y - t^8.65/y + (2*t^8.7)/y - t^3.94*y - t^4.88*y - t^6.3*y - t^6.65*y - t^6.77*y - t^6.94*y - t^7.24*y - t^7.29*y - t^7.59*y - t^7.71*y - t^7.88*y + t^8.06*y + t^8.18*y - t^8.23*y + t^8.35*y - t^8.65*y + 2*t^8.7*y + t^8.83*y^2 | t^2.35/g1^5 + g1^7*t^2.7 + t^2.83/g1^6 + t^3. + g1^12*t^3.35 + g1^5*t^3.65 + t^3.94/g1^2 + g1^4*t^4.12 + g1^10*t^4.29 + 2*g1^3*t^4.59 + t^4.71/g1^10 + t^4.88/g1^4 + g1^15*t^4.94 + g1^2*t^5.06 + t^5.18/g1^11 + 2*g1^8*t^5.23 + g1^14*t^5.41 + 2*g1*t^5.53 + t^5.65/g1^12 + g1^7*t^5.7 + t^5.83/g1^6 + g1^13*t^5.88 - t^6. + g1^19*t^6.05 + 2*g1^6*t^6.17 - t^6.3/g1^7 + 2*g1^12*t^6.35 + (2*t^6.47)/g1 + g1^18*t^6.52 + g1^5*t^6.65 + g1^24*t^6.7 + t^6.77/g1^8 + 2*g1^11*t^6.82 + (2*t^6.94)/g1^2 + 2*g1^17*t^6.99 + t^7.06/g1^15 + 3*g1^4*t^7.12 + 4*g1^10*t^7.29 + (4*t^7.41)/g1^3 + g1^16*t^7.46 + t^7.54/g1^16 + 3*g1^3*t^7.59 + 2*g1^22*t^7.64 + t^7.71/g1^10 + 2*g1^9*t^7.76 + (2*t^7.88)/g1^4 + 5*g1^15*t^7.94 + t^8.01/g1^17 + g1^2*t^8.06 + g1^21*t^8.11 - t^8.18/g1^11 + 6*g1^8*t^8.23 + g1^27*t^8.28 - t^8.35/g1^5 + g1^14*t^8.41 + t^8.48/g1^18 + 3*g1*t^8.53 + 5*g1^20*t^8.58 - g1^7*t^8.7 + g1^26*t^8.75 + t^8.83/g1^6 + 8*g1^13*t^8.88 + t^8.83/(g1^6*y^2) - t^3.94/(g1^2*y) - t^4.88/(g1^4*y) - t^6.3/(g1^7*y) - (g1^5*t^6.65)/y - t^6.77/(g1^8*y) - t^6.94/(g1^2*y) - t^7.24/(g1^9*y) - (g1^10*t^7.29)/y - (g1^3*t^7.59)/y - t^7.71/(g1^10*y) - t^7.88/(g1^4*y) + (g1^2*t^8.06)/y + t^8.18/(g1^11*y) - (g1^8*t^8.23)/y + t^8.35/(g1^5*y) - t^8.65/(g1^12*y) + (2*g1^7*t^8.7)/y - (t^3.94*y)/g1^2 - (t^4.88*y)/g1^4 - (t^6.3*y)/g1^7 - g1^5*t^6.65*y - (t^6.77*y)/g1^8 - (t^6.94*y)/g1^2 - (t^7.24*y)/g1^9 - g1^10*t^7.29*y - g1^3*t^7.59*y - (t^7.71*y)/g1^10 - (t^7.88*y)/g1^4 + g1^2*t^8.06*y + (t^8.18*y)/g1^11 - g1^8*t^8.23*y + (t^8.35*y)/g1^5 - (t^8.65*y)/g1^12 + 2*g1^7*t^8.7*y + (t^8.83*y^2)/g1^6 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 57413 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.4334 | 1.6275 | 0.8807 | [X:[1.3462], M:[0.8172], q:[0.5801, 0.436], qb:[0.4199, 0.6027], phi:[0.3269]] | t^2.452 + t^2.568 + t^2.942 + t^3. + t^3.116 + t^3.548 + t^3.981 + t^4.039 + t^4.097 + 2*t^4.529 + t^4.903 + t^4.961 + t^5.019 + t^5.077 + t^5.135 + t^5.308 + t^5.337 + t^5.394 + 2*t^5.51 + t^5.568 + t^5.684 + t^5.769 + t^5.856 + t^5.884 + t^5.942 - 2*t^6. - t^3.981/y - t^4.961/y - t^3.981*y - t^4.961*y | detail |