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 |
|---|---|---|---|---|---|---|---|---|---|
| 46783 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ | 0.5615 | 0.7236 | 0.776 | [M:[0.6841, 1.1484, 0.9808, 0.7225], q:[0.2967, 1.0192], qb:[0.5549, 0.4258], phi:[0.4258]] | [M:[[11], [-2], [7], [-3]], q:[[-4], [-7]], qb:[[6], [1]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}^{4}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ | ${}M_{4}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | -2 | t^2.052 + 2*t^2.168 + t^2.555 + 2*t^2.942 + 2*t^3.445 + t^4.104 + 2*t^4.22 + 4*t^4.335 + t^4.607 + 3*t^4.723 + 2*t^4.994 + 4*t^5.11 + 3*t^5.497 + 3*t^5.613 + 3*t^5.885 - 2*t^6. + t^6.156 + 2*t^6.272 + 5*t^6.387 + 4*t^6.503 + t^6.659 + 2*t^6.775 + 4*t^6.89 + 2*t^7.047 + 4*t^7.162 + 5*t^7.277 - t^7.393 + 3*t^7.549 + 5*t^7.665 + 3*t^7.78 + 3*t^7.937 + 3*t^8.052 - 6*t^8.168 + t^8.209 + 2*t^8.324 + 6*t^8.44 + 2*t^8.555 + 4*t^8.67 + t^8.711 + 6*t^8.827 - 4*t^8.942 - t^4.277/y - t^6.33/y - t^6.445/y + t^7.22/y + (2*t^7.335)/y + t^7.607/y + (2*t^7.723)/y + (2*t^7.994)/y + (5*t^8.11)/y + t^8.225/y - t^8.382/y + (3*t^8.497)/y + (3*t^8.613)/y + t^8.885/y - t^4.277*y - t^6.33*y - t^6.445*y + t^7.22*y + 2*t^7.335*y + t^7.607*y + 2*t^7.723*y + 2*t^7.994*y + 5*t^8.11*y + t^8.225*y - t^8.382*y + 3*t^8.497*y + 3*t^8.613*y + t^8.885*y | g1^11*t^2.052 + (2*t^2.168)/g1^3 + g1^2*t^2.555 + 2*g1^7*t^2.942 + (2*t^3.445)/g1^2 + g1^22*t^4.104 + 2*g1^8*t^4.22 + (4*t^4.335)/g1^6 + g1^13*t^4.607 + (3*t^4.723)/g1 + 2*g1^18*t^4.994 + 4*g1^4*t^5.11 + 3*g1^9*t^5.497 + (3*t^5.613)/g1^5 + 3*g1^14*t^5.885 - 2*t^6. + g1^33*t^6.156 + 2*g1^19*t^6.272 + 5*g1^5*t^6.387 + (4*t^6.503)/g1^9 + g1^24*t^6.659 + 2*g1^10*t^6.775 + (4*t^6.89)/g1^4 + 2*g1^29*t^7.047 + 4*g1^15*t^7.162 + 5*g1*t^7.277 - t^7.393/g1^13 + 3*g1^20*t^7.549 + 5*g1^6*t^7.665 + (3*t^7.78)/g1^8 + 3*g1^25*t^7.937 + 3*g1^11*t^8.052 - (6*t^8.168)/g1^3 + g1^44*t^8.209 + 2*g1^30*t^8.324 + 6*g1^16*t^8.44 + 2*g1^2*t^8.555 + (4*t^8.67)/g1^12 + g1^35*t^8.711 + 6*g1^21*t^8.827 - 4*g1^7*t^8.942 - (g1*t^4.277)/y - (g1^12*t^6.33)/y - t^6.445/(g1^2*y) + (g1^8*t^7.22)/y + (2*t^7.335)/(g1^6*y) + (g1^13*t^7.607)/y + (2*t^7.723)/(g1*y) + (2*g1^18*t^7.994)/y + (5*g1^4*t^8.11)/y + t^8.225/(g1^10*y) - (g1^23*t^8.382)/y + (3*g1^9*t^8.497)/y + (3*t^8.613)/(g1^5*y) + (g1^14*t^8.885)/y - g1*t^4.277*y - g1^12*t^6.33*y - (t^6.445*y)/g1^2 + g1^8*t^7.22*y + (2*t^7.335*y)/g1^6 + g1^13*t^7.607*y + (2*t^7.723*y)/g1 + 2*g1^18*t^7.994*y + 5*g1^4*t^8.11*y + (t^8.225*y)/g1^10 - g1^23*t^8.382*y + 3*g1^9*t^8.497*y + (3*t^8.613*y)/g1^5 + g1^14*t^8.885*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46213 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ | 0.5415 | 0.6866 | 0.7886 | [M:[0.6781, 1.1494, 0.977], q:[0.2989, 1.023], qb:[0.5517, 0.4253], phi:[0.4253]] | t^2.034 + t^2.172 + t^2.552 + 2*t^2.931 + 2*t^3.448 + t^3.828 + t^4.069 + t^4.207 + 2*t^4.345 + t^4.586 + 2*t^4.724 + 2*t^4.965 + 2*t^5.103 + 3*t^5.483 + t^5.621 + 4*t^5.862 - t^6. - t^4.276/y - t^4.276*y | detail |