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 |
|---|---|---|---|---|---|---|---|---|---|
| 56597 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{7}$ + ${ }M_{1}M_{6}$ + ${ }M_{5}X_{1}$ | 0.6679 | 0.8359 | 0.7991 | [X:[1.3435], M:[1.1348, 1.1043, 0.8652, 0.687, 0.6565, 0.8652, 0.8957], q:[0.3435, 0.5217], qb:[0.5522, 0.7913], phi:[0.4478]] | [X:[[3]], M:[[7], [-2], [-7], [6], [-3], [-7], [2]], q:[[3], [-10]], qb:[[-1], [4]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ | ${}M_{4}\phi_{1}q_{1}q_{2}$ | -2 | t^2.061 + 2*t^2.596 + 2*t^2.687 + t^3.222 + t^3.404 + t^3.939 + 2*t^4.03 + t^4.122 + t^4.474 + t^4.565 + 2*t^4.657 + 3*t^4.748 + 2*t^5.191 + 5*t^5.283 + 3*t^5.374 + 2*t^5.817 + t^5.909 - 2*t^6. + 4*t^6.091 + t^6.183 + t^6.443 + t^6.535 + 4*t^6.626 + 3*t^6.717 + 2*t^6.809 + 2*t^7.069 + 4*t^7.161 + 4*t^7.252 + 2*t^7.343 + 5*t^7.435 + t^7.695 + 2*t^7.787 + 5*t^7.878 + 6*t^7.97 + 2*t^8.152 + t^8.244 + 3*t^8.413 + 4*t^8.504 - 4*t^8.596 - 3*t^8.687 + 7*t^8.778 + 2*t^8.87 + t^8.947 - t^4.343/y - t^6.404/y - t^6.939/y - t^7.03/y + (3*t^7.657)/y + (3*t^7.748)/y + t^8.191/y + (6*t^8.283)/y + t^8.374/y + (2*t^8.817)/y + (2*t^8.909)/y - t^4.343*y - t^6.404*y - t^6.939*y - t^7.03*y + 3*t^7.657*y + 3*t^7.748*y + t^8.191*y + 6*t^8.283*y + t^8.374*y + 2*t^8.817*y + 2*t^8.909*y | g1^6*t^2.061 + (2*t^2.596)/g1^7 + 2*g1^2*t^2.687 + t^3.222/g1^11 + g1^7*t^3.404 + t^3.939/g1^6 + 2*g1^3*t^4.03 + g1^12*t^4.122 + t^4.474/g1^19 + t^4.565/g1^10 + (2*t^4.657)/g1 + 3*g1^8*t^4.748 + (2*t^5.191)/g1^14 + (5*t^5.283)/g1^5 + 3*g1^4*t^5.374 + (2*t^5.817)/g1^18 + t^5.909/g1^9 - 2*t^6. + 4*g1^9*t^6.091 + g1^18*t^6.183 + t^6.443/g1^22 + t^6.535/g1^13 + (4*t^6.626)/g1^4 + 3*g1^5*t^6.717 + 2*g1^14*t^6.809 + (2*t^7.069)/g1^26 + (4*t^7.161)/g1^17 + (4*t^7.252)/g1^8 + 2*g1*t^7.343 + 5*g1^10*t^7.435 + t^7.695/g1^30 + (2*t^7.787)/g1^21 + (5*t^7.878)/g1^12 + (6*t^7.97)/g1^3 + 2*g1^15*t^8.152 + g1^24*t^8.244 + (3*t^8.413)/g1^25 + (4*t^8.504)/g1^16 - (4*t^8.596)/g1^7 - 3*g1^2*t^8.687 + 7*g1^11*t^8.778 + 2*g1^20*t^8.87 + t^8.947/g1^38 - (g1*t^4.343)/y - (g1^7*t^6.404)/y - t^6.939/(g1^6*y) - (g1^3*t^7.03)/y + (3*t^7.657)/(g1*y) + (3*g1^8*t^7.748)/y + t^8.191/(g1^14*y) + (6*t^8.283)/(g1^5*y) + (g1^4*t^8.374)/y + (2*t^8.817)/(g1^18*y) + (2*t^8.909)/(g1^9*y) - g1*t^4.343*y - g1^7*t^6.404*y - (t^6.939*y)/g1^6 - g1^3*t^7.03*y + (3*t^7.657*y)/g1 + 3*g1^8*t^7.748*y + (t^8.191*y)/g1^14 + (6*t^8.283*y)/g1^5 + g1^4*t^8.374*y + (2*t^8.817*y)/g1^18 + (2*t^8.909*y)/g1^9 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 54585 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{7}$ | 0.735 | 0.921 | 0.7981 | [M:[1.0277, 1.0526, 0.9723, 0.8422, 0.867, 0.6841, 0.9474], q:[0.4211, 0.5512], qb:[0.5263, 0.6066], phi:[0.4737]] | t^2.052 + t^2.527 + t^2.601 + 2*t^2.842 + t^2.917 + t^3.083 + t^3.232 + t^4.105 + t^4.263 + t^4.338 + t^4.504 + 2*t^4.579 + 2*t^4.654 + t^4.728 + t^4.82 + 3*t^4.895 + t^4.969 + t^5.053 + t^5.061 + t^5.128 + t^5.136 + t^5.202 + t^5.285 + 2*t^5.369 + 2*t^5.443 + t^5.518 + 3*t^5.684 + 2*t^5.759 + t^5.834 + t^5.925 - 3*t^6. - t^4.421/y - t^4.421*y | detail |