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 |
|---|---|---|---|---|---|---|---|---|---|
| 46930 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{1}M_{5}$ | 0.5723 | 0.7114 | 0.8045 | [M:[1.061, 0.939, 0.6951, 1.183, 0.939], q:[0.6128, 0.3262], qb:[0.4482, 0.9787], phi:[0.4085]] | [M:[[4], [-4], [-20], [12], [-4]], q:[[-9], [5]], qb:[[13], [15]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$ | ${}M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ | 0 | t^2.085 + t^2.323 + 2*t^2.817 + t^3.183 + 2*t^3.549 + t^3.915 + t^4.17 + t^4.281 + t^4.409 + t^4.647 + t^4.774 + 2*t^4.902 + 2*t^5.14 + t^5.506 + 3*t^5.634 + 2*t^5.872 + t^6.238 + t^6.255 + 3*t^6.366 + t^6.604 + 2*t^6.732 - t^6.86 + t^6.97 + 2*t^6.987 + 4*t^7.098 + 3*t^7.464 - t^7.591 + 3*t^7.719 + 3*t^7.83 + t^7.957 - 2*t^8.085 + 3*t^8.196 + t^8.341 + 3*t^8.451 + 2*t^8.562 + 2*t^8.689 - 4*t^8.817 + t^8.927 - t^4.226/y - t^6.311/y - t^7.043/y + (2*t^7.409)/y + (2*t^7.902)/y + (3*t^8.14)/y + t^8.268/y - t^8.396/y + t^8.506/y + (3*t^8.634)/y + (2*t^8.872)/y - t^4.226*y - t^6.311*y - t^7.043*y + 2*t^7.409*y + 2*t^7.902*y + 3*t^8.14*y + t^8.268*y - t^8.396*y + t^8.506*y + 3*t^8.634*y + 2*t^8.872*y | t^2.085/g1^20 + g1^18*t^2.323 + (2*t^2.817)/g1^4 + g1^4*t^3.183 + 2*g1^12*t^3.549 + g1^20*t^3.915 + t^4.17/g1^40 + g1^28*t^4.281 + t^4.409/g1^2 + g1^36*t^4.647 + g1^6*t^4.774 + (2*t^4.902)/g1^24 + 2*g1^14*t^5.14 + g1^22*t^5.506 + (3*t^5.634)/g1^8 + 2*g1^30*t^5.872 + g1^38*t^6.238 + t^6.255/g1^60 + 3*g1^8*t^6.366 + g1^46*t^6.604 + 2*g1^16*t^6.732 - t^6.86/g1^14 + g1^54*t^6.97 + (2*t^6.987)/g1^44 + 4*g1^24*t^7.098 + 3*g1^32*t^7.464 - g1^2*t^7.591 + (3*t^7.719)/g1^28 + 3*g1^40*t^7.83 + g1^10*t^7.957 - (2*t^8.085)/g1^20 + 3*g1^48*t^8.196 + t^8.341/g1^80 + (3*t^8.451)/g1^12 + 2*g1^56*t^8.562 + 2*g1^26*t^8.689 - (4*t^8.817)/g1^4 + g1^64*t^8.927 - t^4.226/(g1^6*y) - t^6.311/(g1^26*y) - t^7.043/(g1^10*y) + (2*t^7.409)/(g1^2*y) + (2*t^7.902)/(g1^24*y) + (3*g1^14*t^8.14)/y + t^8.268/(g1^16*y) - t^8.396/(g1^46*y) + (g1^22*t^8.506)/y + (3*t^8.634)/(g1^8*y) + (2*g1^30*t^8.872)/y - (t^4.226*y)/g1^6 - (t^6.311*y)/g1^26 - (t^7.043*y)/g1^10 + (2*t^7.409*y)/g1^2 + (2*t^7.902*y)/g1^24 + 3*g1^14*t^8.14*y + (t^8.268*y)/g1^16 - (t^8.396*y)/g1^46 + g1^22*t^8.506*y + (3*t^8.634*y)/g1^8 + 2*g1^30*t^8.872*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 |
|---|---|---|---|---|---|---|---|---|
| 55255 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ | 0.5929 | 0.7511 | 0.7894 | [M:[1.0622, 0.9378, 0.6888, 1.1867, 0.9378, 0.6888], q:[0.6099, 0.3278], qb:[0.4523, 0.9834], phi:[0.4066]] | 2*t^2.066 + t^2.34 + 2*t^2.813 + t^3.187 + 2*t^3.56 + 3*t^4.133 + t^4.307 + 2*t^4.407 + t^4.681 + t^4.78 + 4*t^4.88 + 2*t^5.154 + t^5.253 + t^5.527 + 5*t^5.627 + 2*t^5.901 - t^6. - t^4.22/y - t^4.22*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46556 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}^{2}$ | 0.5667 | 0.7026 | 0.8065 | [M:[1.0591, 0.9409, 0.7045, 1.1773], q:[0.617, 0.3239], qb:[0.442, 0.9716], phi:[0.4114]] | t^2.114 + t^2.298 + t^2.823 + 2*t^3.177 + 2*t^3.532 + t^3.886 + t^4.227 + t^4.241 + t^4.411 + t^4.595 + t^4.766 + t^4.936 + t^5.12 + t^5.291 + 2*t^5.475 + t^5.645 + 2*t^5.83 - t^4.234/y - t^4.234*y | detail |