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 |
|---|---|---|---|---|---|---|---|---|---|
| 55421 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}^{2}$ | 0.6433 | 0.7961 | 0.8081 | [M:[1.1553, 0.8894, 0.8447, 0.7106, 0.7553, 1.2], q:[0.3553, 0.4894], qb:[0.7553, 0.8], phi:[0.4]] | [M:[[1], [-2], [-1], [2], [1], [0]], q:[[1], [-2]], qb:[[1], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{5}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}$, ${ }M_{6}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{4}\phi_{1}q_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{5}\phi_{1}q_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}$ | -1 | t^2.132 + t^2.266 + t^2.534 + t^2.668 + t^3.332 + t^3.466 + t^3.6 + t^3.734 + t^4.136 + t^4.264 + t^4.398 + 2*t^4.532 + 2*t^4.666 + t^4.8 + 2*t^4.934 + t^5.068 + t^5.336 + t^5.464 + t^5.598 + 3*t^5.732 + 2*t^5.866 - t^6. + t^6.134 + 2*t^6.268 + t^6.395 + t^6.529 + 3*t^6.664 + t^6.671 + 3*t^6.798 + t^6.805 + 2*t^6.932 + 3*t^7.066 + 2*t^7.2 + 2*t^7.468 + t^7.595 + 2*t^7.602 + t^7.729 + 4*t^7.864 + t^7.871 + 4*t^7.998 + t^8.005 - t^8.132 + t^8.273 + 2*t^8.4 + t^8.527 - 2*t^8.534 + t^8.661 - t^8.668 + 3*t^8.795 + t^8.802 + 3*t^8.929 - t^4.2/y - t^6.332/y - t^6.466/y - t^6.868/y + t^7.398/y + t^7.532/y + t^7.666/y + (2*t^7.8)/y + (2*t^7.934)/y + t^8.068/y + t^8.202/y + t^8.598/y + t^8.732/y + (3*t^8.866)/y - t^4.2*y - t^6.332*y - t^6.466*y - t^6.868*y + t^7.398*y + t^7.532*y + t^7.666*y + 2*t^7.8*y + 2*t^7.934*y + t^8.068*y + t^8.202*y + t^8.598*y + t^8.732*y + 3*t^8.866*y | g1^2*t^2.132 + g1*t^2.266 + t^2.534/g1 + t^2.668/g1^2 + g1^2*t^3.332 + g1*t^3.466 + t^3.6 + t^3.734/g1 + t^4.136/g1^4 + g1^4*t^4.264 + g1^3*t^4.398 + 2*g1^2*t^4.532 + 2*g1*t^4.666 + t^4.8 + (2*t^4.934)/g1 + t^5.068/g1^2 + t^5.336/g1^4 + g1^4*t^5.464 + g1^3*t^5.598 + 3*g1^2*t^5.732 + 2*g1*t^5.866 - t^6. + t^6.134/g1 + (2*t^6.268)/g1^2 + g1^6*t^6.395 + g1^5*t^6.529 + 3*g1^4*t^6.664 + t^6.671/g1^5 + 3*g1^3*t^6.798 + t^6.805/g1^6 + 2*g1^2*t^6.932 + 3*g1*t^7.066 + 2*t^7.2 + (2*t^7.468)/g1^2 + g1^6*t^7.595 + (2*t^7.602)/g1^3 + g1^5*t^7.729 + 4*g1^4*t^7.864 + t^7.871/g1^5 + 4*g1^3*t^7.998 + t^8.005/g1^6 - g1^2*t^8.132 + t^8.273/g1^8 + 2*t^8.4 + g1^8*t^8.527 - (2*t^8.534)/g1 + g1^7*t^8.661 - t^8.668/g1^2 + 3*g1^6*t^8.795 + t^8.802/g1^3 + 3*g1^5*t^8.929 - t^4.2/y - (g1^2*t^6.332)/y - (g1*t^6.466)/y - t^6.868/(g1^2*y) + (g1^3*t^7.398)/y + (g1^2*t^7.532)/y + (g1*t^7.666)/y + (2*t^7.8)/y + (2*t^7.934)/(g1*y) + t^8.068/(g1^2*y) + t^8.202/(g1^3*y) + (g1^3*t^8.598)/y + (g1^2*t^8.732)/y + (3*g1*t^8.866)/y - t^4.2*y - g1^2*t^6.332*y - g1*t^6.466*y - (t^6.868*y)/g1^2 + g1^3*t^7.398*y + g1^2*t^7.532*y + g1*t^7.666*y + 2*t^7.8*y + (2*t^7.934*y)/g1 + (t^8.068*y)/g1^2 + (t^8.202*y)/g1^3 + g1^3*t^8.598*y + g1^2*t^8.732*y + 3*g1*t^8.866*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47066 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ | 0.6598 | 0.8251 | 0.7997 | [M:[1.1553, 0.8894, 0.8447, 0.7106, 0.7553], q:[0.3553, 0.4894], qb:[0.7553, 0.8], phi:[0.4]] | t^2.132 + t^2.266 + t^2.4 + t^2.534 + t^2.668 + t^3.332 + t^3.466 + t^3.734 + t^4.136 + t^4.264 + t^4.398 + 3*t^4.532 + 3*t^4.666 + 2*t^4.8 + 3*t^4.934 + 2*t^5.068 + t^5.336 + t^5.464 + t^5.598 + 3*t^5.732 + 2*t^5.866 - t^6. - t^4.2/y - t^4.2*y | detail |