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 |
|---|---|---|---|---|---|---|---|---|---|
| 1973 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$ | 0.6655 | 0.8456 | 0.787 | [M:[0.8272, 1.2, 0.7728, 0.8, 0.7728, 0.7456], q:[0.8, 0.3728], qb:[0.8, 0.4272], phi:[0.4]] | [M:[[1], [0], [-1], [0], [-1], [-2]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{2}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{3}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{6}q_{1}q_{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{5}q_{1}q_{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{5}$, ${ }M_{4}q_{1}q_{2}$ | ${}\phi_{1}\tilde{q}_{1}^{2}$ | 0 | t^2.237 + 2*t^2.318 + 2*t^2.4 + t^2.482 + t^3.437 + t^3.518 + t^3.6 + t^4.474 + 2*t^4.555 + 5*t^4.637 + 5*t^4.718 + 6*t^4.8 + 2*t^4.882 + t^4.963 + t^5.674 + 3*t^5.755 + 4*t^5.837 + 3*t^5.918 - t^6.082 - t^6.163 + t^6.711 + 2*t^6.792 + 6*t^6.874 + 10*t^6.955 + 12*t^7.037 + 10*t^7.118 + 7*t^7.2 + 2*t^7.282 + t^7.445 + t^7.911 + 3*t^7.992 + 7*t^8.074 + 8*t^8.155 + 6*t^8.237 - 2*t^8.318 - 5*t^8.4 - 8*t^8.482 - 4*t^8.563 - t^8.645 + t^8.947 - t^4.2/y - t^6.437/y - (2*t^6.518)/y - t^6.6/y - t^6.682/y + (2*t^7.555)/y + (3*t^7.637)/y + (6*t^7.718)/y + (4*t^7.8)/y + (4*t^7.882)/y + t^7.963/y + t^8.755/y + t^8.837/y + (2*t^8.918)/y - t^4.2*y - t^6.437*y - 2*t^6.518*y - t^6.6*y - t^6.682*y + 2*t^7.555*y + 3*t^7.637*y + 6*t^7.718*y + 4*t^7.8*y + 4*t^7.882*y + t^7.963*y + t^8.755*y + t^8.837*y + 2*t^8.918*y | t^2.237/g1^2 + (2*t^2.318)/g1 + 2*t^2.4 + g1*t^2.482 + t^3.437/g1^2 + t^3.518/g1 + t^3.6 + t^4.474/g1^4 + (2*t^4.555)/g1^3 + (5*t^4.637)/g1^2 + (5*t^4.718)/g1 + 6*t^4.8 + 2*g1*t^4.882 + g1^2*t^4.963 + t^5.674/g1^4 + (3*t^5.755)/g1^3 + (4*t^5.837)/g1^2 + (3*t^5.918)/g1 - g1*t^6.082 - g1^2*t^6.163 + t^6.711/g1^6 + (2*t^6.792)/g1^5 + (6*t^6.874)/g1^4 + (10*t^6.955)/g1^3 + (12*t^7.037)/g1^2 + (10*t^7.118)/g1 + 7*t^7.2 + 2*g1*t^7.282 + g1^3*t^7.445 + t^7.911/g1^6 + (3*t^7.992)/g1^5 + (7*t^8.074)/g1^4 + (8*t^8.155)/g1^3 + (6*t^8.237)/g1^2 - (2*t^8.318)/g1 - 5*t^8.4 - 8*g1*t^8.482 - 4*g1^2*t^8.563 - g1^3*t^8.645 + t^8.947/g1^8 - t^4.2/y - t^6.437/(g1^2*y) - (2*t^6.518)/(g1*y) - t^6.6/y - (g1*t^6.682)/y + (2*t^7.555)/(g1^3*y) + (3*t^7.637)/(g1^2*y) + (6*t^7.718)/(g1*y) + (4*t^7.8)/y + (4*g1*t^7.882)/y + (g1^2*t^7.963)/y + t^8.755/(g1^3*y) + t^8.837/(g1^2*y) + (2*t^8.918)/(g1*y) - t^4.2*y - (t^6.437*y)/g1^2 - (2*t^6.518*y)/g1 - t^6.6*y - g1*t^6.682*y + (2*t^7.555*y)/g1^3 + (3*t^7.637*y)/g1^2 + (6*t^7.718*y)/g1 + 4*t^7.8*y + 4*g1*t^7.882*y + g1^2*t^7.963*y + (t^8.755*y)/g1^3 + (t^8.837*y)/g1^2 + (2*t^8.918*y)/g1 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 666 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ | 0.6469 | 0.8101 | 0.7985 | [M:[0.8118, 1.2, 0.7882, 0.8, 0.7882], q:[0.8, 0.3882], qb:[0.8, 0.4118], phi:[0.4]] | 2*t^2.365 + 2*t^2.4 + t^2.435 + t^3.529 + t^3.565 + t^3.6 + t^3.671 + 3*t^4.729 + 4*t^4.765 + 6*t^4.8 + 2*t^4.835 + t^4.871 + 2*t^5.894 + 3*t^5.929 + 3*t^5.965 - t^4.2/y - t^4.2*y | detail |