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 |
|---|---|---|---|---|---|---|---|---|---|
| 57640 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{3}M_{7}$ | 0.6881 | 0.8524 | 0.8073 | [M:[0.9518, 1.0209, 1.1172, 0.7448, 0.8138, 1.0482, 0.8828], q:[0.5722, 0.4759], qb:[0.4069, 0.7793], phi:[0.4414]] | [M:[[-22], [-32], [12], [8], [-2], [22], [-12]], q:[[33], [-11]], qb:[[-1], [3]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{5}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{6}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$ | ${}$ | -2 | t^2.234 + t^2.441 + 2*t^2.648 + t^3.063 + t^3.144 + t^3.766 + t^3.973 + t^4.055 + t^4.18 + t^4.262 + 2*t^4.469 + t^4.676 + t^4.758 + 3*t^4.883 + 2*t^5.09 + 4*t^5.297 + t^5.379 + t^5.586 + t^5.711 + t^5.793 - 2*t^6. + t^6.125 + t^6.207 + t^6.289 + 3*t^6.414 + t^6.496 + 2*t^6.621 + 3*t^6.703 + 2*t^6.828 + 3*t^6.91 + t^6.992 + 3*t^7.117 + 2*t^7.199 + t^7.242 + 2*t^7.324 + 2*t^7.406 + 5*t^7.531 + 3*t^7.738 + t^7.902 + 6*t^7.945 + 2*t^8.027 - t^8.234 + 3*t^8.36 - t^8.441 + 2*t^8.523 + t^8.567 - 3*t^8.648 + t^8.73 + t^8.774 + t^8.812 + t^8.856 + 3*t^8.937 - t^4.324/y - t^6.559/y - t^6.766/y - t^6.973/y + t^7.262/y - t^7.387/y + (2*t^7.676)/y + (3*t^7.883)/y + (3*t^8.09)/y + (2*t^8.297)/y + t^8.379/y + t^8.504/y + t^8.586/y + (2*t^8.711)/y + t^8.793/y - t^4.324*y - t^6.559*y - t^6.766*y - t^6.973*y + t^7.262*y - t^7.387*y + 2*t^7.676*y + 3*t^7.883*y + 3*t^8.09*y + 2*t^8.297*y + t^8.379*y + t^8.504*y + t^8.586*y + 2*t^8.711*y + t^8.793*y | g1^8*t^2.234 + t^2.441/g1^2 + (2*t^2.648)/g1^12 + t^3.063/g1^32 + g1^22*t^3.144 + t^3.766/g1^8 + t^3.973/g1^18 + g1^36*t^4.055 + t^4.18/g1^28 + g1^26*t^4.262 + 2*g1^16*t^4.469 + g1^6*t^4.676 + g1^60*t^4.758 + (3*t^4.883)/g1^4 + (2*t^5.09)/g1^14 + (4*t^5.297)/g1^24 + g1^30*t^5.379 + g1^20*t^5.586 + t^5.711/g1^44 + g1^10*t^5.793 - 2*t^6. + t^6.125/g1^64 + t^6.207/g1^10 + g1^44*t^6.289 + (3*t^6.414)/g1^20 + g1^34*t^6.496 + (2*t^6.621)/g1^30 + 3*g1^24*t^6.703 + (2*t^6.828)/g1^40 + 3*g1^14*t^6.91 + g1^68*t^6.992 + 3*g1^4*t^7.117 + 2*g1^58*t^7.199 + t^7.242/g1^60 + (2*t^7.324)/g1^6 + 2*g1^48*t^7.406 + (5*t^7.531)/g1^16 + (3*t^7.738)/g1^26 + g1^82*t^7.902 + (6*t^7.945)/g1^36 + 2*g1^18*t^8.027 - g1^8*t^8.234 + (3*t^8.36)/g1^56 - t^8.441/g1^2 + 2*g1^52*t^8.523 + t^8.567/g1^66 - (3*t^8.648)/g1^12 + g1^42*t^8.73 + t^8.774/g1^76 + g1^96*t^8.812 + t^8.856/g1^22 + 3*g1^32*t^8.937 - t^4.324/(g1^6*y) - (g1^2*t^6.559)/y - t^6.766/(g1^8*y) - t^6.973/(g1^18*y) + (g1^26*t^7.262)/y - t^7.387/(g1^38*y) + (2*g1^6*t^7.676)/y + (3*t^7.883)/(g1^4*y) + (3*t^8.09)/(g1^14*y) + (2*t^8.297)/(g1^24*y) + (g1^30*t^8.379)/y + t^8.504/(g1^34*y) + (g1^20*t^8.586)/y + (2*t^8.711)/(g1^44*y) + (g1^10*t^8.793)/y - (t^4.324*y)/g1^6 - g1^2*t^6.559*y - (t^6.766*y)/g1^8 - (t^6.973*y)/g1^18 + g1^26*t^7.262*y - (t^7.387*y)/g1^38 + 2*g1^6*t^7.676*y + (3*t^7.883*y)/g1^4 + (3*t^8.09*y)/g1^14 + (2*t^8.297*y)/g1^24 + g1^30*t^8.379*y + (t^8.504*y)/g1^34 + g1^20*t^8.586*y + (2*t^8.711*y)/g1^44 + g1^10*t^8.793*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 |
|---|---|---|---|---|---|---|---|---|---|
| 55934 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{6}$ | 0.6779 | 0.8353 | 0.8115 | [M:[0.9634, 1.0377, 1.1109, 0.7406, 0.8149, 1.0366], q:[0.5549, 0.4817], qb:[0.4074, 0.7777], phi:[0.4446]] | t^2.222 + t^2.445 + t^2.667 + t^3.11 + t^3.113 + t^3.333 + t^3.778 + t^3.998 + t^4.001 + t^4.221 + t^4.224 + 2*t^4.444 + t^4.663 + t^4.666 + 2*t^4.889 + t^5.112 + t^5.332 + 2*t^5.335 + 2*t^5.554 + t^5.777 - t^6. - t^4.334/y - t^4.334*y | detail |