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 |
|---|---|---|---|---|---|---|---|---|---|
| 46541 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6082 | 0.781 | 0.7787 | [M:[0.9798, 0.9798, 0.7652, 1.0606], q:[0.7449, 0.2753], qb:[0.4899, 0.4495], phi:[0.5101]] | [M:[[4], [4], [-3], [-12]], q:[[1], [-5]], qb:[[2], [10]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{2}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }M_{2}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}M_{3}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.174 + 2*t^2.295 + 2*t^2.939 + 2*t^3.182 + t^3.583 + t^3.705 + t^3.826 + t^4.227 + 2*t^4.348 + 3*t^4.47 + 3*t^4.591 + 2*t^5.114 + 4*t^5.235 + t^5.356 + 3*t^5.477 + t^5.758 + 4*t^5.879 - t^6. + 3*t^6.121 + 3*t^6.364 + t^6.401 + 4*t^6.523 + 3*t^6.644 + 5*t^6.765 + 3*t^6.886 + t^7.008 + 2*t^7.167 + 3*t^7.288 + 4*t^7.409 + 5*t^7.53 + 2*t^7.652 + 4*t^7.773 + t^7.811 + 2*t^7.932 + 3*t^8.053 + 3*t^8.174 - 3*t^8.295 + 3*t^8.417 + t^8.454 + t^8.538 + 2*t^8.576 + 4*t^8.659 + 5*t^8.697 + 7*t^8.818 - 2*t^8.939 - t^4.53/y - t^6.826/y + t^7.348/y + t^7.47/y + (2*t^7.591)/y - t^7.712/y + (2*t^8.114)/y + (5*t^8.235)/y + (2*t^8.356)/y + (4*t^8.477)/y + t^8.758/y + (4*t^8.879)/y - t^4.53*y - t^6.826*y + t^7.348*y + t^7.47*y + 2*t^7.591*y - t^7.712*y + 2*t^8.114*y + 5*t^8.235*y + 2*t^8.356*y + 4*t^8.477*y + t^8.758*y + 4*t^8.879*y | g1^5*t^2.174 + (2*t^2.295)/g1^3 + 2*g1^4*t^2.939 + (2*t^3.182)/g1^12 + g1^11*t^3.583 + g1^3*t^3.705 + t^3.826/g1^5 + g1^18*t^4.227 + 2*g1^10*t^4.348 + 3*g1^2*t^4.47 + (3*t^4.591)/g1^6 + 2*g1^9*t^5.114 + 4*g1*t^5.235 + t^5.356/g1^7 + (3*t^5.477)/g1^15 + g1^16*t^5.758 + 4*g1^8*t^5.879 - t^6. + (3*t^6.121)/g1^8 + (3*t^6.364)/g1^24 + g1^23*t^6.401 + 4*g1^15*t^6.523 + 3*g1^7*t^6.644 + (5*t^6.765)/g1 + (3*t^6.886)/g1^9 + t^7.008/g1^17 + 2*g1^22*t^7.167 + 3*g1^14*t^7.288 + 4*g1^6*t^7.409 + (5*t^7.53)/g1^2 + (2*t^7.652)/g1^10 + (4*t^7.773)/g1^18 + g1^29*t^7.811 + 2*g1^21*t^7.932 + 3*g1^13*t^8.053 + 3*g1^5*t^8.174 - (3*t^8.295)/g1^3 + (3*t^8.417)/g1^11 + g1^36*t^8.454 + t^8.538/g1^19 + 2*g1^28*t^8.576 + (4*t^8.659)/g1^27 + 5*g1^20*t^8.697 + 7*g1^12*t^8.818 - 2*g1^4*t^8.939 - t^4.53/(g1^2*y) - t^6.826/(g1^5*y) + (g1^10*t^7.348)/y + (g1^2*t^7.47)/y + (2*t^7.591)/(g1^6*y) - t^7.712/(g1^14*y) + (2*g1^9*t^8.114)/y + (5*g1*t^8.235)/y + (2*t^8.356)/(g1^7*y) + (4*t^8.477)/(g1^15*y) + (g1^16*t^8.758)/y + (4*g1^8*t^8.879)/y - (t^4.53*y)/g1^2 - (t^6.826*y)/g1^5 + g1^10*t^7.348*y + g1^2*t^7.47*y + (2*t^7.591*y)/g1^6 - (t^7.712*y)/g1^14 + 2*g1^9*t^8.114*y + 5*g1*t^8.235*y + (2*t^8.356*y)/g1^7 + (4*t^8.477*y)/g1^15 + g1^16*t^8.758*y + 4*g1^8*t^8.879*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46152 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ | 0.616 | 0.7963 | 0.7736 | [M:[0.964, 0.964, 0.777], q:[0.741, 0.295], qb:[0.482, 0.41], phi:[0.518]] | t^2.115 + 2*t^2.331 + t^2.676 + 2*t^2.892 + t^3.324 + t^3.453 + t^3.669 + t^3.885 + t^4.014 + 2*t^4.23 + 3*t^4.446 + 3*t^4.662 + t^4.791 + 4*t^5.007 + 4*t^5.223 + t^5.352 + 3*t^5.568 + t^5.655 + 4*t^5.784 - t^4.554/y - t^4.554*y | detail |