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 |
|---|---|---|---|---|---|---|---|---|---|
| 46618 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ | 0.6051 | 0.7764 | 0.7793 | [M:[0.9973, 1.0082, 1.0027, 0.7575], q:[0.7493, 0.2534], qb:[0.4932, 0.4986], phi:[0.5014]] | [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 |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{4}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}\phi_{1}q_{2}^{2}$ | ${}\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | -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 | g1^5*t^2.24 + t^2.256/g1^3 + t^2.273/g1^11 + (2*t^3.008)/g1^4 + (2*t^3.025)/g1^12 + 2*g1^3*t^3.744 + t^3.76/g1^5 + g1^18*t^4.463 + 2*g1^10*t^4.479 + 2*g1^2*t^4.496 + (2*t^4.512)/g1^6 + t^4.529/g1^14 + t^4.545/g1^22 + 2*g1*t^5.248 + (3*t^5.264)/g1^7 + (3*t^5.281)/g1^15 + (2*t^5.297)/g1^23 - t^6. + (3*t^6.016)/g1^8 + (5*t^6.033)/g1^16 + (3*t^6.049)/g1^24 + g1^23*t^6.703 + g1^15*t^6.719 + (4*t^6.752)/g1 + (6*t^6.768)/g1^9 + (3*t^6.785)/g1^17 + t^6.801/g1^25 + t^6.818/g1^33 - g1^22*t^7.455 + 3*g1^6*t^7.488 + (4*t^7.504)/g1^2 + (5*t^7.521)/g1^10 + (4*t^7.537)/g1^18 + (3*t^7.553)/g1^26 + (2*t^7.57)/g1^34 + g1^21*t^8.207 - g1^13*t^8.223 - 3*g1^5*t^8.24 + (2*t^8.273)/g1^11 + (6*t^8.289)/g1^19 + (6*t^8.305)/g1^27 + (3*t^8.322)/g1^35 + g1^36*t^8.926 + 2*g1^28*t^8.943 + 2*g1^20*t^8.959 - g1^4*t^8.992 - t^4.504/(g1^2*y) - t^6.777/(g1^13*y) + (g1^10*t^7.479)/y + (2*g1^2*t^7.496)/y + (g1^9*t^8.232)/y + (2*g1*t^8.248)/y + (4*t^8.264)/(g1^7*y) + (4*t^8.281)/(g1^15*y) + (2*t^8.297)/(g1^23*y) + (2*g1^8*t^8.984)/y - (t^4.504*y)/g1^2 - (t^6.777*y)/g1^13 + g1^10*t^7.479*y + 2*g1^2*t^7.496*y + g1^9*t^8.232*y + 2*g1*t^8.248*y + (4*t^8.264*y)/g1^7 + (4*t^8.281*y)/g1^15 + (2*t^8.297*y)/g1^23 + 2*g1^8*t^8.984*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46103 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ | 0.6056 | 0.7771 | 0.7792 | [M:[0.9925, 1.0225, 1.0075, 0.7511], q:[0.7481, 0.2594], qb:[0.5008, 0.4768], phi:[0.5037]] | t^2.208 + t^2.253 + t^2.28 + 2*t^3.022 + 2*t^3.067 + t^3.675 + t^3.72 + t^3.792 + t^4.372 + t^4.417 + t^4.444 + t^4.462 + t^4.489 + t^4.507 + t^4.516 + t^4.534 + t^4.561 + 2*t^5.231 + 3*t^5.276 + 2*t^5.303 + 2*t^5.321 + t^5.348 + t^5.883 + t^5.928 + t^5.973 - 2*t^6. - t^4.511/y - t^4.511*y | detail |