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 |
|---|---|---|---|---|---|---|---|---|---|
| 3593 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.5878 | 0.7405 | 0.7937 | [X:[1.5704], M:[0.4296, 1.2887, 0.7113, 1.0071, 0.9929, 0.845, 0.8592], q:[0.926, 0.6444], qb:[0.3627, 0.3486], phi:[0.4296]] | [X:[[2]], M:[[-2], [-6], [6], [-14], [14], [24], [-4]], q:[[5], [-3]], qb:[[-11], [17]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{4}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{5}M_{6}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{7}\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$ | ${}$ | -1 | t^2.134 + t^2.535 + 2*t^2.577 + t^2.979 + t^3.021 + t^3.38 + t^3.824 + t^3.866 + t^4.268 + t^4.669 + 3*t^4.711 + t^5.07 + 3*t^5.113 + 4*t^5.155 + 2*t^5.514 + 2*t^5.556 + t^5.599 + t^5.915 + 3*t^5.958 - t^6. + 2*t^6.359 + 3*t^6.401 + t^6.76 + t^6.803 + t^6.845 - t^6.887 + 2*t^7.204 + 3*t^7.246 + 3*t^7.289 - t^7.331 + t^7.605 + 5*t^7.648 + 5*t^7.69 + 5*t^7.732 + 2*t^8.049 + 5*t^8.091 - t^8.134 + t^8.45 + 4*t^8.493 + 3*t^8.535 - 5*t^8.577 - t^8.62 + 3*t^8.894 + 4*t^8.936 - t^4.289/y - t^6.824/y - (2*t^6.866)/y + t^7.669/y + (4*t^7.711)/y + t^7.754/y + (3*t^8.113)/y + (2*t^8.155)/y + (2*t^8.514)/y + (3*t^8.556)/y + (2*t^8.599)/y + t^8.915/y + (3*t^8.958)/y - t^4.289*y - t^6.824*y - 2*t^6.866*y + t^7.669*y + 4*t^7.711*y + t^7.754*y + 3*t^8.113*y + 2*t^8.155*y + 2*t^8.514*y + 3*t^8.556*y + 2*t^8.599*y + t^8.915*y + 3*t^8.958*y | g1^6*t^2.134 + g1^24*t^2.535 + (2*t^2.577)/g1^4 + g1^14*t^2.979 + t^3.021/g1^14 + g1^32*t^3.38 + g1^22*t^3.824 + t^3.866/g1^6 + g1^12*t^4.268 + g1^30*t^4.669 + 3*g1^2*t^4.711 + g1^48*t^5.07 + 3*g1^20*t^5.113 + (4*t^5.155)/g1^8 + 2*g1^38*t^5.514 + 2*g1^10*t^5.556 + t^5.599/g1^18 + g1^56*t^5.915 + 3*g1^28*t^5.958 - t^6. + 2*g1^46*t^6.359 + 3*g1^18*t^6.401 + g1^64*t^6.76 + g1^36*t^6.803 + g1^8*t^6.845 - t^6.887/g1^20 + 2*g1^54*t^7.204 + 3*g1^26*t^7.246 + (3*t^7.289)/g1^2 - t^7.331/g1^30 + g1^72*t^7.605 + 5*g1^44*t^7.648 + 5*g1^16*t^7.69 + (5*t^7.732)/g1^12 + 2*g1^62*t^8.049 + 5*g1^34*t^8.091 - g1^6*t^8.134 + g1^80*t^8.45 + 4*g1^52*t^8.493 + 3*g1^24*t^8.535 - (5*t^8.577)/g1^4 - t^8.62/g1^32 + 3*g1^70*t^8.894 + 4*g1^42*t^8.936 - t^4.289/(g1^2*y) - (g1^22*t^6.824)/y - (2*t^6.866)/(g1^6*y) + (g1^30*t^7.669)/y + (4*g1^2*t^7.711)/y + t^7.754/(g1^26*y) + (3*g1^20*t^8.113)/y + (2*t^8.155)/(g1^8*y) + (2*g1^38*t^8.514)/y + (3*g1^10*t^8.556)/y + (2*t^8.599)/(g1^18*y) + (g1^56*t^8.915)/y + (3*g1^28*t^8.958)/y - (t^4.289*y)/g1^2 - g1^22*t^6.824*y - (2*t^6.866*y)/g1^6 + g1^30*t^7.669*y + 4*g1^2*t^7.711*y + (t^7.754*y)/g1^26 + 3*g1^20*t^8.113*y + (2*t^8.155*y)/g1^8 + 2*g1^38*t^8.514*y + 3*g1^10*t^8.556*y + (2*t^8.599*y)/g1^18 + g1^56*t^8.915*y + 3*g1^28*t^8.958*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2984 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ | 0.5754 | 0.7199 | 0.7992 | [X:[1.5698], M:[0.4302, 1.2905, 0.7095, 1.0111, 0.9889, 0.8382], q:[0.9246, 0.6452], qb:[0.3658, 0.3437], phi:[0.4302]] | t^2.129 + t^2.515 + t^2.581 + t^2.967 + t^3.033 + t^3.353 + t^3.419 + t^3.805 + t^3.871 + t^4.257 + t^4.643 + 2*t^4.71 + t^5.029 + 2*t^5.095 + 2*t^5.162 + 2*t^5.481 + 2*t^5.548 + t^5.867 + 3*t^5.934 - t^4.29/y - t^4.29*y | detail |