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 |
|---|---|---|---|---|---|---|---|---|---|
| 46873 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ | 0.6385 | 0.8121 | 0.7862 | [M:[1.1113, 0.75, 0.7226, 1.25, 0.8887], q:[0.75, 0.3887], qb:[0.3613, 0.5], phi:[0.5]] | [M:[[1], [0], [2], [0], [-1]], q:[[0], [-1]], qb:[[1], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{2}$, ${ }M_{3}q_{1}q_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}q_{1}q_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$ | ${}M_{2}M_{4}$, ${ }M_{1}M_{5}$ | 1 | t^2.168 + t^2.25 + t^2.584 + t^2.666 + t^3. + t^3.334 + t^3.416 + t^3.668 + 2*t^3.75 + t^4.084 + t^4.166 + t^4.336 + t^4.418 + 2*t^4.5 + t^4.752 + 2*t^4.834 + t^4.916 + 2*t^5.168 + 2*t^5.25 + t^5.332 + t^5.502 + 2*t^5.584 + t^5.666 + t^5.836 + 3*t^5.918 + t^6. + 2*t^6.252 + 3*t^6.334 + t^6.416 + t^6.504 + t^6.586 + 4*t^6.668 + 3*t^6.75 + t^6.832 + t^6.92 + 3*t^7.002 + 3*t^7.084 + t^7.166 + 3*t^7.336 + 4*t^7.418 + 3*t^7.5 + t^7.67 + 4*t^7.752 + 3*t^7.834 + t^7.916 + t^7.998 + t^8.004 + 3*t^8.086 + 3*t^8.168 + t^8.25 + 2*t^8.42 + 4*t^8.502 + t^8.584 - t^8.666 + t^8.672 + t^8.754 + 5*t^8.836 + 4*t^8.918 - t^4.5/y - t^6.668/y + t^7.418/y + t^7.752/y + (2*t^7.834)/y + t^7.916/y + t^8.168/y + (2*t^8.25)/y + t^8.332/y + t^8.502/y + (3*t^8.584)/y + (2*t^8.666)/y + (4*t^8.918)/y - t^4.5*y - t^6.668*y + t^7.418*y + t^7.752*y + 2*t^7.834*y + t^7.916*y + t^8.168*y + 2*t^8.25*y + t^8.332*y + t^8.502*y + 3*t^8.584*y + 2*t^8.666*y + 4*t^8.918*y | g1^2*t^2.168 + t^2.25 + g1*t^2.584 + t^2.666/g1 + t^3. + g1*t^3.334 + t^3.416/g1 + g1^2*t^3.668 + 2*t^3.75 + g1*t^4.084 + t^4.166/g1 + g1^4*t^4.336 + g1^2*t^4.418 + 2*t^4.5 + g1^3*t^4.752 + 2*g1*t^4.834 + t^4.916/g1 + 2*g1^2*t^5.168 + 2*t^5.25 + t^5.332/g1^2 + g1^3*t^5.502 + 2*g1*t^5.584 + t^5.666/g1 + g1^4*t^5.836 + 3*g1^2*t^5.918 + t^6. + 2*g1^3*t^6.252 + 3*g1*t^6.334 + t^6.416/g1 + g1^6*t^6.504 + g1^4*t^6.586 + 4*g1^2*t^6.668 + 3*t^6.75 + t^6.832/g1^2 + g1^5*t^6.92 + 3*g1^3*t^7.002 + 3*g1*t^7.084 + t^7.166/g1 + 3*g1^4*t^7.336 + 4*g1^2*t^7.418 + 3*t^7.5 + g1^5*t^7.67 + 4*g1^3*t^7.752 + 3*g1*t^7.834 + t^7.916/g1 + t^7.998/g1^3 + g1^6*t^8.004 + 3*g1^4*t^8.086 + 3*g1^2*t^8.168 + t^8.25 + 2*g1^5*t^8.42 + 4*g1^3*t^8.502 + g1*t^8.584 - t^8.666/g1 + g1^8*t^8.672 + g1^6*t^8.754 + 5*g1^4*t^8.836 + 4*g1^2*t^8.918 - t^4.5/y - (g1^2*t^6.668)/y + (g1^2*t^7.418)/y + (g1^3*t^7.752)/y + (2*g1*t^7.834)/y + t^7.916/(g1*y) + (g1^2*t^8.168)/y + (2*t^8.25)/y + t^8.332/(g1^2*y) + (g1^3*t^8.502)/y + (3*g1*t^8.584)/y + (2*t^8.666)/(g1*y) + (4*g1^2*t^8.918)/y - t^4.5*y - g1^2*t^6.668*y + g1^2*t^7.418*y + g1^3*t^7.752*y + 2*g1*t^7.834*y + (t^7.916*y)/g1 + g1^2*t^8.168*y + 2*t^8.25*y + (t^8.332*y)/g1^2 + g1^3*t^8.502*y + 3*g1*t^8.584*y + (2*t^8.666*y)/g1 + 4*g1^2*t^8.918*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46712 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ | 0.629 | 0.7983 | 0.788 | [M:[1.0975, 0.75, 0.6949, 1.25], q:[0.75, 0.4025], qb:[0.3475, 0.5], phi:[0.5]] | t^2.085 + t^2.25 + t^2.542 + t^3. + 2*t^3.292 + t^3.458 + t^3.585 + 2*t^3.75 + t^4.042 + t^4.17 + t^4.208 + t^4.335 + 2*t^4.5 + t^4.627 + t^4.792 + 2*t^5.085 + t^5.25 + 2*t^5.377 + 3*t^5.542 + t^5.67 + 4*t^5.835 - t^4.5/y - t^4.5*y | detail |