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 |
|---|---|---|---|---|---|---|---|---|---|
| 2097 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{6}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ | 0.6051 | 0.7764 | 0.7793 | [M:[1.0082, 0.9973, 0.7575, 1.2479, 0.7521, 1.0027], q:[0.4932, 0.4986], qb:[0.7493, 0.2534], phi:[0.5014]] | [M:[[12], [-4], [11], [-3], [3], [4]], q:[[-10], [-2]], qb:[[-1], [5]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{2}$, ${ }M_{5}$, ${ }M_{3}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ | ${}M_{5}\phi_{1}q_{1}\tilde{q}_{2}$ | -1 | t^2.24 + t^2.256 + t^2.273 + 2*t^3.008 + 2*t^3.025 + 2*t^3.744 + t^3.76 + t^4.463 + 2*t^4.479 + 2*t^4.496 + 2*t^4.512 + t^4.529 + t^4.545 + 2*t^5.248 + 3*t^5.264 + 3*t^5.281 + 2*t^5.297 - t^6. + 3*t^6.016 + 5*t^6.033 + 3*t^6.049 + t^6.703 + t^6.719 + 4*t^6.752 + 6*t^6.768 + 3*t^6.785 + t^6.801 + t^6.818 - t^7.455 + 3*t^7.488 + 4*t^7.504 + 5*t^7.521 + 4*t^7.537 + 3*t^7.553 + 2*t^7.57 + t^8.207 - t^8.223 - 3*t^8.24 + 2*t^8.273 + 6*t^8.289 + 6*t^8.305 + 3*t^8.322 + t^8.926 + 2*t^8.943 + 2*t^8.959 - t^8.992 - t^4.504/y - t^6.777/y + t^7.479/y + (2*t^7.496)/y + t^8.232/y + (2*t^8.248)/y + (4*t^8.264)/y + (4*t^8.281)/y + (2*t^8.297)/y + (2*t^8.984)/y - t^4.504*y - t^6.777*y + t^7.479*y + 2*t^7.496*y + t^8.232*y + 2*t^8.248*y + 4*t^8.264*y + 4*t^8.281*y + 2*t^8.297*y + 2*t^8.984*y | t^2.24/g1^5 + g1^3*t^2.256 + g1^11*t^2.273 + 2*g1^4*t^3.008 + 2*g1^12*t^3.025 + (2*t^3.744)/g1^3 + g1^5*t^3.76 + t^4.463/g1^18 + (2*t^4.479)/g1^10 + (2*t^4.496)/g1^2 + 2*g1^6*t^4.512 + g1^14*t^4.529 + g1^22*t^4.545 + (2*t^5.248)/g1 + 3*g1^7*t^5.264 + 3*g1^15*t^5.281 + 2*g1^23*t^5.297 - t^6. + 3*g1^8*t^6.016 + 5*g1^16*t^6.033 + 3*g1^24*t^6.049 + t^6.703/g1^23 + t^6.719/g1^15 + 4*g1*t^6.752 + 6*g1^9*t^6.768 + 3*g1^17*t^6.785 + g1^25*t^6.801 + g1^33*t^6.818 - t^7.455/g1^22 + (3*t^7.488)/g1^6 + 4*g1^2*t^7.504 + 5*g1^10*t^7.521 + 4*g1^18*t^7.537 + 3*g1^26*t^7.553 + 2*g1^34*t^7.57 + t^8.207/g1^21 - t^8.223/g1^13 - (3*t^8.24)/g1^5 + 2*g1^11*t^8.273 + 6*g1^19*t^8.289 + 6*g1^27*t^8.305 + 3*g1^35*t^8.322 + t^8.926/g1^36 + (2*t^8.943)/g1^28 + (2*t^8.959)/g1^20 - t^8.992/g1^4 - (g1^2*t^4.504)/y - (g1^13*t^6.777)/y + t^7.479/(g1^10*y) + (2*t^7.496)/(g1^2*y) + t^8.232/(g1^9*y) + (2*t^8.248)/(g1*y) + (4*g1^7*t^8.264)/y + (4*g1^15*t^8.281)/y + (2*g1^23*t^8.297)/y + (2*t^8.984)/(g1^8*y) - g1^2*t^4.504*y - g1^13*t^6.777*y + (t^7.479*y)/g1^10 + (2*t^7.496*y)/g1^2 + (t^8.232*y)/g1^9 + (2*t^8.248*y)/g1 + 4*g1^7*t^8.264*y + 4*g1^15*t^8.281*y + 2*g1^23*t^8.297*y + (2*t^8.984*y)/g1^8 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 959 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{6}$ | 0.7153 | 0.8822 | 0.8108 | [M:[0.822, 1.0593, 0.8597, 1.0216, 0.9784, 0.9407], q:[0.6484, 0.5297], qb:[0.4919, 0.4488], phi:[0.4703]] | t^2.466 + t^2.579 + 2*t^2.822 + t^2.935 + t^3.065 + t^3.291 + t^4.103 + t^4.233 + t^4.346 + t^4.362 + t^4.476 + t^4.589 + t^4.702 + t^4.832 + t^4.932 + t^4.945 + t^5.045 + t^5.158 + 2*t^5.288 + t^5.301 + 2*t^5.401 + t^5.514 + 3*t^5.644 + 2*t^5.757 + t^5.871 + t^5.887 - 3*t^6. - t^4.411/y - t^4.411*y | detail |