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 |
|---|---|---|---|---|---|---|---|---|---|
| 56988 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{7}$ | 0.6635 | 0.8279 | 0.8015 | [M:[0.9627, 1.1701, 1.0816, 0.8299, 0.8741, 0.7109, 1.0373], q:[0.4744, 0.5629], qb:[0.3555, 0.7704], phi:[0.4592]] | [M:[[-10], [-8], [4], [8], [2], [-6], [10]], q:[[11], [-1]], qb:[[-3], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{7}$, ${ }M_{3}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{4}M_{7}$, ${ }M_{3}M_{4}$, ${ }M_{5}M_{7}$, ${ }M_{3}M_{5}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$ | ${}$ | -1 | t^2.133 + t^2.49 + t^2.622 + t^2.755 + t^3.112 + t^3.245 + t^3.51 + t^3.734 + t^4. + t^4.133 + t^4.224 + t^4.266 + t^4.49 + t^4.622 + 2*t^4.755 + t^4.888 + t^4.979 + t^5.112 + 3*t^5.245 + t^5.378 + t^5.51 + t^5.602 + t^5.734 + 3*t^5.867 - t^6. + t^6.133 + 2*t^6.224 + t^6.266 + 2*t^6.357 + t^6.398 + t^6.49 + t^6.622 + t^6.713 + t^6.755 + 2*t^6.846 + 2*t^6.888 + 2*t^6.979 + t^7.021 + t^7.112 + 3*t^7.245 + t^7.336 + 2*t^7.378 + 2*t^7.469 + 2*t^7.51 + t^7.602 + t^7.643 + 3*t^7.734 + 2*t^7.867 + t^7.958 + 3*t^8. + t^8.091 - 2*t^8.133 + 2*t^8.224 + 2*t^8.266 + 3*t^8.357 + t^8.448 + 2*t^8.49 + t^8.531 - t^8.622 + 3*t^8.713 - t^8.755 + 2*t^8.846 + 5*t^8.979 - t^4.378/y - t^6.51/y - t^7./y + t^7.622/y + (2*t^7.755)/y + t^7.888/y + t^8.112/y + (3*t^8.245)/y + (2*t^8.378)/y + t^8.602/y + (2*t^8.734)/y + (3*t^8.867)/y - t^4.378*y - t^6.51*y - t^7.*y + t^7.622*y + 2*t^7.755*y + t^7.888*y + t^8.112*y + 3*t^8.245*y + 2*t^8.378*y + t^8.602*y + 2*t^8.734*y + 3*t^8.867*y | t^2.133/g1^6 + g1^8*t^2.49 + g1^2*t^2.622 + t^2.755/g1^4 + g1^10*t^3.112 + g1^4*t^3.245 + t^3.51/g1^8 + g1^12*t^3.734 + t^4. + t^4.133/g1^6 + g1^20*t^4.224 + t^4.266/g1^12 + g1^8*t^4.49 + g1^2*t^4.622 + (2*t^4.755)/g1^4 + t^4.888/g1^10 + g1^16*t^4.979 + g1^10*t^5.112 + 3*g1^4*t^5.245 + t^5.378/g1^2 + t^5.51/g1^8 + g1^18*t^5.602 + g1^12*t^5.734 + 3*g1^6*t^5.867 - t^6. + t^6.133/g1^6 + 2*g1^20*t^6.224 + t^6.266/g1^12 + 2*g1^14*t^6.357 + t^6.398/g1^18 + g1^8*t^6.49 + g1^2*t^6.622 + g1^28*t^6.713 + t^6.755/g1^4 + 2*g1^22*t^6.846 + (2*t^6.888)/g1^10 + 2*g1^16*t^6.979 + t^7.021/g1^16 + g1^10*t^7.112 + 3*g1^4*t^7.245 + g1^30*t^7.336 + (2*t^7.378)/g1^2 + 2*g1^24*t^7.469 + (2*t^7.51)/g1^8 + g1^18*t^7.602 + t^7.643/g1^14 + 3*g1^12*t^7.734 + 2*g1^6*t^7.867 + g1^32*t^7.958 + 3*t^8. + g1^26*t^8.091 - (2*t^8.133)/g1^6 + 2*g1^20*t^8.224 + (2*t^8.266)/g1^12 + 3*g1^14*t^8.357 + g1^40*t^8.448 + 2*g1^8*t^8.49 + t^8.531/g1^24 - g1^2*t^8.622 + 3*g1^28*t^8.713 - t^8.755/g1^4 + 2*g1^22*t^8.846 + 5*g1^16*t^8.979 - t^4.378/(g1^2*y) - t^6.51/(g1^8*y) - t^7./y + (g1^2*t^7.622)/y + (2*t^7.755)/(g1^4*y) + t^7.888/(g1^10*y) + (g1^10*t^8.112)/y + (3*g1^4*t^8.245)/y + (2*t^8.378)/(g1^2*y) + (g1^18*t^8.602)/y + (2*g1^12*t^8.734)/y + (3*g1^6*t^8.867)/y - (t^4.378*y)/g1^2 - (t^6.51*y)/g1^8 - t^7.*y + g1^2*t^7.622*y + (2*t^7.755*y)/g1^4 + (t^7.888*y)/g1^10 + g1^10*t^8.112*y + 3*g1^4*t^8.245*y + (2*t^8.378*y)/g1^2 + g1^18*t^8.602*y + 2*g1^12*t^8.734*y + 3*g1^6*t^8.867*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 |
|---|---|---|---|---|---|---|---|---|---|
| 55375 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}\tilde{q}_{1}$ | 0.6686 | 0.8353 | 0.8005 | [M:[0.9278, 1.1423, 1.0955, 0.8577, 0.8811, 0.69], q:[0.5127, 0.5595], qb:[0.345, 0.7739], phi:[0.4522]] | t^2.07 + t^2.573 + t^2.643 + t^2.713 + t^2.784 + t^3.287 + t^3.427 + t^3.86 + t^4. + t^4.07 + t^4.14 + t^4.433 + t^4.573 + t^4.643 + 2*t^4.713 + t^4.784 + t^4.854 + t^5.146 + t^5.216 + 2*t^5.287 + 2*t^5.357 + 2*t^5.427 + t^5.497 + t^5.567 + 2*t^5.93 - t^6. - t^4.357/y - t^4.357*y | detail |