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 |
|---|---|---|---|---|---|---|---|---|---|
| 55980 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{3}M_{6}$ | 0.6657 | 0.8235 | 0.8084 | [M:[1.1475, 0.9836, 1.082, 0.8525, 0.7869, 0.918], q:[0.4754, 0.3771], qb:[0.541, 0.7705], phi:[0.459]] | [M:[[-5], [-13], [4], [5], [14], [-4]], q:[[11], [-6]], qb:[[2], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{4}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}^{2}$ | ${}$ | -2 | t^2.361 + t^2.557 + 2*t^2.754 + t^2.951 + t^3.443 + t^3.738 + 2*t^3.934 + t^4.131 + t^4.229 + t^4.426 + t^4.623 + t^4.721 + t^4.918 + 3*t^5.115 + 3*t^5.311 + 3*t^5.508 + t^5.705 + t^5.902 - 2*t^6. + t^6.098 + 2*t^6.295 + t^6.393 + 2*t^6.492 + t^6.59 + 3*t^6.689 + 2*t^6.787 + 2*t^6.885 + 3*t^6.984 + t^7.082 + t^7.18 + t^7.279 + t^7.377 + 3*t^7.475 + 4*t^7.672 + 5*t^7.869 + t^7.967 + 4*t^8.066 + 2*t^8.164 + 4*t^8.262 - 2*t^8.361 + 3*t^8.459 - 3*t^8.557 + 4*t^8.656 - 4*t^8.754 + 3*t^8.852 + t^8.853 - 2*t^8.951 - t^4.377/y - t^6.738/y - t^7.131/y - t^7.328/y + t^7.426/y + t^7.623/y + t^7.918/y + t^8.016/y + (2*t^8.115)/y + (3*t^8.311)/y + (2*t^8.508)/y + (2*t^8.705)/y + t^8.803/y - t^4.377*y - t^6.738*y - t^7.131*y - t^7.328*y + t^7.426*y + t^7.623*y + t^7.918*y + t^8.016*y + 2*t^8.115*y + 3*t^8.311*y + 2*t^8.508*y + 2*t^8.705*y + t^8.803*y | g1^14*t^2.361 + g1^5*t^2.557 + (2*t^2.754)/g1^4 + t^2.951/g1^13 + t^3.443/g1^5 + g1^12*t^3.738 + 2*g1^3*t^3.934 + t^4.131/g1^6 + g1^20*t^4.229 + g1^11*t^4.426 + g1^2*t^4.623 + g1^28*t^4.721 + g1^19*t^4.918 + 3*g1^10*t^5.115 + 3*g1*t^5.311 + (3*t^5.508)/g1^8 + t^5.705/g1^17 + t^5.902/g1^26 - 2*t^6. + g1^26*t^6.098 + 2*g1^17*t^6.295 + t^6.393/g1^18 + 2*g1^8*t^6.492 + g1^34*t^6.59 + (3*t^6.689)/g1 + 2*g1^25*t^6.787 + (2*t^6.885)/g1^10 + 3*g1^16*t^6.984 + g1^42*t^7.082 + g1^7*t^7.18 + g1^33*t^7.279 + t^7.377/g1^2 + 3*g1^24*t^7.475 + 4*g1^15*t^7.672 + 5*g1^6*t^7.869 + g1^32*t^7.967 + (4*t^8.066)/g1^3 + 2*g1^23*t^8.164 + (4*t^8.262)/g1^12 - 2*g1^14*t^8.361 + t^8.459/g1^21 + 2*g1^40*t^8.459 - 3*g1^5*t^8.557 + t^8.656/g1^30 + 3*g1^31*t^8.656 - (4*t^8.754)/g1^4 + 3*g1^22*t^8.852 + t^8.853/g1^39 - (3*t^8.951)/g1^13 + g1^48*t^8.951 - t^4.377/(g1^2*y) - (g1^12*t^6.738)/y - t^7.131/(g1^6*y) - t^7.328/(g1^15*y) + (g1^11*t^7.426)/y + (g1^2*t^7.623)/y + (g1^19*t^7.918)/y + t^8.016/(g1^16*y) + (2*g1^10*t^8.115)/y + (3*g1*t^8.311)/y + (2*t^8.508)/(g1^8*y) + (2*t^8.705)/(g1^17*y) + (g1^9*t^8.803)/y - (t^4.377*y)/g1^2 - g1^12*t^6.738*y - (t^7.131*y)/g1^6 - (t^7.328*y)/g1^15 + g1^11*t^7.426*y + g1^2*t^7.623*y + g1^19*t^7.918*y + (t^8.016*y)/g1^16 + 2*g1^10*t^8.115*y + 3*g1*t^8.311*y + (2*t^8.508*y)/g1^8 + (2*t^8.705*y)/g1^17 + g1^9*t^8.803*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 |
|---|---|---|---|---|---|---|---|---|---|
| 48267 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ | 0.6584 | 0.8119 | 0.8109 | [M:[1.1521, 0.9956, 1.0783, 0.8479, 0.774], q:[0.4653, 0.3826], qb:[0.5391, 0.7696], phi:[0.4609]] | t^2.322 + t^2.544 + t^2.765 + t^2.987 + t^3.235 + t^3.456 + t^3.705 + 2*t^3.926 + t^4.148 + t^4.174 + t^4.396 + t^4.617 + t^4.644 + t^4.866 + 2*t^5.087 + 2*t^5.309 + t^5.53 + t^5.557 + t^5.778 + t^5.973 - t^6. - t^4.383/y - t^4.383*y | detail |