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 |
|---|---|---|---|---|---|---|---|---|---|
| 2732 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ | 0.6065 | 0.7774 | 0.7802 | [M:[0.9872, 1.0385, 0.9872, 0.7853], q:[0.7468, 0.266], qb:[0.4679, 0.4936], phi:[0.5064]] | [M:[[4], [-12], [4], [-11]], q:[[1], [-5]], qb:[[10], [2]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{4}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$ | ${}\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.202 + t^2.279 + t^2.356 + 2*t^2.961 + 2*t^3.116 + 2*t^3.721 + t^3.798 + t^4.327 + 2*t^4.404 + 2*t^4.481 + 2*t^4.558 + t^4.635 + t^4.712 + 2*t^5.163 + 2*t^5.24 + 3*t^5.317 + t^5.394 + 2*t^5.471 + 3*t^5.923 - t^6. + 4*t^6.077 + t^6.154 + 3*t^6.231 + t^6.529 + t^6.606 + 4*t^6.683 + 2*t^6.76 + 4*t^6.837 + 3*t^6.914 + t^6.991 + t^7.068 + t^7.288 + 2*t^7.365 + 3*t^7.442 + 4*t^7.519 + 3*t^7.596 + 4*t^7.673 + t^7.75 + 2*t^7.827 + t^8.048 + 2*t^8.125 + 2*t^8.279 - t^8.356 + 5*t^8.433 + 2*t^8.51 + 3*t^8.587 + t^8.653 + 2*t^8.73 + 2*t^8.807 + 4*t^8.884 - 3*t^8.961 - t^4.519/y - t^6.875/y + t^7.404/y + (2*t^7.558)/y + (3*t^8.163)/y + (2*t^8.24)/y + (4*t^8.317)/y + (2*t^8.394)/y + (2*t^8.471)/y + (3*t^8.923)/y - t^4.519*y - t^6.875*y + t^7.404*y + 2*t^7.558*y + 3*t^8.163*y + 2*t^8.24*y + 4*t^8.317*y + 2*t^8.394*y + 2*t^8.471*y + 3*t^8.923*y | g1^5*t^2.202 + t^2.279/g1^3 + t^2.356/g1^11 + 2*g1^4*t^2.961 + (2*t^3.116)/g1^12 + 2*g1^3*t^3.721 + t^3.798/g1^5 + g1^18*t^4.327 + 2*g1^10*t^4.404 + 2*g1^2*t^4.481 + (2*t^4.558)/g1^6 + t^4.635/g1^14 + t^4.712/g1^22 + 2*g1^9*t^5.163 + 2*g1*t^5.24 + (3*t^5.317)/g1^7 + t^5.394/g1^15 + (2*t^5.471)/g1^23 + 3*g1^8*t^5.923 - t^6. + (4*t^6.077)/g1^8 + t^6.154/g1^16 + (3*t^6.231)/g1^24 + g1^23*t^6.529 + g1^15*t^6.606 + 4*g1^7*t^6.683 + (2*t^6.76)/g1 + (4*t^6.837)/g1^9 + (3*t^6.914)/g1^17 + t^6.991/g1^25 + t^7.068/g1^33 + g1^22*t^7.288 + 2*g1^14*t^7.365 + 3*g1^6*t^7.442 + (4*t^7.519)/g1^2 + (3*t^7.596)/g1^10 + (4*t^7.673)/g1^18 + t^7.75/g1^26 + (2*t^7.827)/g1^34 + g1^21*t^8.048 + 2*g1^13*t^8.125 + (2*t^8.279)/g1^3 - t^8.356/g1^11 + (5*t^8.433)/g1^19 + (2*t^8.51)/g1^27 + (3*t^8.587)/g1^35 + g1^36*t^8.653 + 2*g1^28*t^8.73 + 2*g1^20*t^8.807 + 4*g1^12*t^8.884 - 3*g1^4*t^8.961 - t^4.519/(g1^2*y) - t^6.875/(g1^13*y) + (g1^10*t^7.404)/y + (2*t^7.558)/(g1^6*y) + (3*g1^9*t^8.163)/y + (2*g1*t^8.24)/y + (4*t^8.317)/(g1^7*y) + (2*t^8.394)/(g1^15*y) + (2*t^8.471)/(g1^23*y) + (3*g1^8*t^8.923)/y - (t^4.519*y)/g1^2 - (t^6.875*y)/g1^13 + g1^10*t^7.404*y + (2*t^7.558*y)/g1^6 + 3*g1^9*t^8.163*y + 2*g1*t^8.24*y + (4*t^8.317*y)/g1^7 + (2*t^8.394*y)/g1^15 + (2*t^8.471*y)/g1^23 + 3*g1^8*t^8.923*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 |
|---|---|---|---|---|---|---|---|---|---|
| 1734 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ | 0.6083 | 0.7807 | 0.7792 | [M:[0.9781, 1.0657, 0.9781, 0.7742], q:[0.7445, 0.2774], qb:[0.4812, 0.453], phi:[0.511]] | t^2.191 + t^2.276 + t^2.323 + 2*t^2.934 + 2*t^3.197 + t^3.593 + t^3.724 + t^3.809 + t^4.251 + t^4.336 + t^4.382 + t^4.42 + t^4.467 + t^4.514 + t^4.552 + t^4.599 + t^4.645 + 2*t^5.125 + 2*t^5.21 + 2*t^5.257 + t^5.388 + t^5.473 + 2*t^5.52 + t^5.784 + 3*t^5.869 + t^5.915 - 2*t^6. - t^4.533/y - t^4.533*y | detail |