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 |
|---|---|---|---|---|---|---|---|---|---|
| 47106 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ | 0.6958 | 0.8515 | 0.8172 | [M:[1.0366, 0.9451, 0.9634, 1.0183, 1.0], q:[0.5092, 0.4542], qb:[0.5458, 0.5275], phi:[0.4908]] | [M:[[4], [-6], [-4], [2], [0]], q:[[1], [-5]], qb:[[5], [3]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{4}$, ${ }M_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{5}\phi_{1}^{2}$ | ${}$ | -1 | t^2.835 + t^2.89 + t^2.945 + t^3. + t^3.055 + t^3.11 + t^3.22 + t^4.198 + t^4.363 + t^4.418 + t^4.473 + t^4.527 + t^4.582 + 2*t^4.637 + t^4.692 + t^4.747 + t^5.67 + t^5.78 + t^5.835 + 2*t^5.89 + t^5.945 - t^6. + t^6.055 + t^6.11 + t^6.165 + t^6.22 + t^6.33 + t^6.439 + t^7.033 + t^7.088 + t^7.143 + t^7.198 + t^7.253 + 2*t^7.308 + 2*t^7.363 + 2*t^7.418 + 2*t^7.473 + 2*t^7.527 + 3*t^7.582 + 3*t^7.637 + 2*t^7.692 + 2*t^7.747 + t^7.802 + 2*t^7.857 + t^7.912 + t^7.967 + t^8.396 + t^8.506 + t^8.561 + t^8.616 + t^8.67 + 2*t^8.725 + t^8.78 + t^8.835 - t^8.945 - t^4.473/y - t^7.308/y + t^7.637/y + t^8.725/y + t^8.78/y + (2*t^8.835)/y + (2*t^8.89)/y + (3*t^8.945)/y - t^4.473*y - t^7.308*y + t^7.637*y + t^8.725*y + t^8.78*y + 2*t^8.835*y + 2*t^8.89*y + 3*t^8.945*y | t^2.835/g1^6 + t^2.89/g1^4 + t^2.945/g1^2 + t^3. + g1^2*t^3.055 + g1^4*t^3.11 + g1^8*t^3.22 + t^4.198/g1^11 + t^4.363/g1^5 + t^4.418/g1^3 + t^4.473/g1 + g1*t^4.527 + g1^3*t^4.582 + 2*g1^5*t^4.637 + g1^7*t^4.692 + g1^9*t^4.747 + t^5.67/g1^12 + t^5.78/g1^8 + t^5.835/g1^6 + (2*t^5.89)/g1^4 + t^5.945/g1^2 - t^6. + g1^2*t^6.055 + g1^4*t^6.11 + g1^6*t^6.165 + g1^8*t^6.22 + g1^12*t^6.33 + g1^16*t^6.439 + t^7.033/g1^17 + t^7.088/g1^15 + t^7.143/g1^13 + t^7.198/g1^11 + t^7.253/g1^9 + (2*t^7.308)/g1^7 + (2*t^7.363)/g1^5 + (2*t^7.418)/g1^3 + (2*t^7.473)/g1 + 2*g1*t^7.527 + 3*g1^3*t^7.582 + 3*g1^5*t^7.637 + 2*g1^7*t^7.692 + 2*g1^9*t^7.747 + g1^11*t^7.802 + 2*g1^13*t^7.857 + g1^15*t^7.912 + g1^17*t^7.967 + t^8.396/g1^22 + t^8.506/g1^18 + t^8.561/g1^16 + t^8.616/g1^14 + t^8.67/g1^12 + (2*t^8.725)/g1^10 + t^8.78/g1^8 + t^8.835/g1^6 - t^8.945/g1^2 - t^4.473/(g1*y) - t^7.308/(g1^7*y) + (g1^5*t^7.637)/y + t^8.725/(g1^10*y) + t^8.78/(g1^8*y) + (2*t^8.835)/(g1^6*y) + (2*t^8.89)/(g1^4*y) + (3*t^8.945)/(g1^2*y) - (t^4.473*y)/g1 - (t^7.308*y)/g1^7 + g1^5*t^7.637*y + (t^8.725*y)/g1^10 + (t^8.78*y)/g1^8 + (2*t^8.835*y)/g1^6 + (2*t^8.89*y)/g1^4 + (3*t^8.945*y)/g1^2 |
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 |
|---|---|---|---|---|---|---|---|---|
| 55480 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{6}\phi_{1}^{2}$ | 0.6943 | 0.8491 | 0.8176 | [M:[1.0295, 0.9557, 0.9705, 1.0148, 1.0, 1.0148], q:[0.5074, 0.4631], qb:[0.5369, 0.5222], phi:[0.4926]] | t^2.867 + t^2.911 + t^3. + 2*t^3.044 + t^3.089 + t^3.177 + t^4.256 + t^4.389 + t^4.434 + t^4.478 + t^4.522 + t^4.566 + 2*t^4.611 + t^4.655 + t^4.699 + t^5.734 + 2*t^5.911 + t^5.956 - 2*t^6. - t^4.478/y - t^4.478*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46681 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ | 0.7101 | 0.8727 | 0.8137 | [M:[0.9774, 0.8432, 1.0226, 1.0523, 0.8729], q:[0.5261, 0.4964], qb:[0.6307, 0.4513], phi:[0.4739]] | t^2.53 + t^2.619 + t^2.843 + t^2.932 + t^3.068 + t^3.157 + t^3.246 + t^4.129 + t^4.265 + t^4.354 + t^4.4 + t^4.489 + t^4.578 + t^4.668 + t^4.803 + t^4.892 + t^5.059 + t^5.148 + t^5.206 + t^5.237 + t^5.373 + t^5.462 + t^5.551 + 2*t^5.686 + 2*t^5.776 + t^5.865 - 2*t^6. - t^4.422/y - t^4.422*y | detail |