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 |
|---|---|---|---|---|---|---|---|---|---|
| 57105 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}M_{6}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6921 | 0.8505 | 0.8137 | [M:[1.0184, 0.9963, 0.9816, 1.011, 0.989, 0.9816, 0.9963], q:[0.5055, 0.4761], qb:[0.4982, 0.5129], phi:[0.5018]] | [M:[[10], [-2], [-10], [6], [-6], [-10], [-2]], q:[[3], [-13]], qb:[[-1], [7]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{5}$, ${ }M_{2}$, ${ }M_{7}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{3}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{7}^{2}$ | ${}$ | -3 | t^2.923 + 2*t^2.945 + t^2.967 + 2*t^2.989 + t^3.033 + t^4.362 + t^4.428 + t^4.45 + t^4.472 + t^4.494 + t^4.517 + 2*t^4.539 + t^4.561 + t^4.583 + t^5.845 + 2*t^5.867 + 3*t^5.89 + 3*t^5.912 + 4*t^5.934 + 2*t^5.956 + 2*t^5.978 - 3*t^6. - t^6.044 - t^6.088 - t^6.11 + t^7.285 + 2*t^7.307 + t^7.329 + 2*t^7.351 + 2*t^7.373 + 3*t^7.395 + 3*t^7.417 + 3*t^7.439 + 4*t^7.461 + 3*t^7.483 + 2*t^7.506 + 3*t^7.528 + t^7.55 + t^7.572 - t^7.594 + t^8.724 + t^8.768 + 3*t^8.79 + 4*t^8.812 + 6*t^8.834 + 5*t^8.856 + 6*t^8.878 + 5*t^8.901 + 2*t^8.923 - 4*t^8.945 - 2*t^8.967 - 6*t^8.989 - t^4.506/y - t^7.45/y - t^7.494/y + t^7.517/y + t^7.561/y + (2*t^8.867)/y + (2*t^8.89)/y + (4*t^8.912)/y + (4*t^8.934)/y + (3*t^8.956)/y + (3*t^8.978)/y - t^4.506*y - t^7.45*y - t^7.494*y + t^7.517*y + t^7.561*y + 2*t^8.867*y + 2*t^8.89*y + 4*t^8.912*y + 4*t^8.934*y + 3*t^8.956*y + 3*t^8.978*y | t^2.923/g1^14 + (2*t^2.945)/g1^10 + t^2.967/g1^6 + (2*t^2.989)/g1^2 + g1^6*t^3.033 + t^4.362/g1^25 + t^4.428/g1^13 + t^4.45/g1^9 + t^4.472/g1^5 + t^4.494/g1 + g1^3*t^4.517 + 2*g1^7*t^4.539 + g1^11*t^4.561 + g1^15*t^4.583 + t^5.845/g1^28 + (2*t^5.867)/g1^24 + (3*t^5.89)/g1^20 + (3*t^5.912)/g1^16 + (4*t^5.934)/g1^12 + (2*t^5.956)/g1^8 + (2*t^5.978)/g1^4 - 3*t^6. - g1^8*t^6.044 - g1^16*t^6.088 - g1^20*t^6.11 + t^7.285/g1^39 + (2*t^7.307)/g1^35 + t^7.329/g1^31 + (2*t^7.351)/g1^27 + (2*t^7.373)/g1^23 + (3*t^7.395)/g1^19 + (3*t^7.417)/g1^15 + (3*t^7.439)/g1^11 + (4*t^7.461)/g1^7 + (3*t^7.483)/g1^3 + 2*g1*t^7.506 + 3*g1^5*t^7.528 + g1^9*t^7.55 + g1^13*t^7.572 - g1^17*t^7.594 + t^8.724/g1^50 + t^8.768/g1^42 + (3*t^8.79)/g1^38 + (4*t^8.812)/g1^34 + (6*t^8.834)/g1^30 + (5*t^8.856)/g1^26 + (6*t^8.878)/g1^22 + (5*t^8.901)/g1^18 + (2*t^8.923)/g1^14 - (4*t^8.945)/g1^10 - (2*t^8.967)/g1^6 - (6*t^8.989)/g1^2 - (g1*t^4.506)/y - t^7.45/(g1^9*y) - t^7.494/(g1*y) + (g1^3*t^7.517)/y + (g1^11*t^7.561)/y + (2*t^8.867)/(g1^24*y) + (2*t^8.89)/(g1^20*y) + (4*t^8.912)/(g1^16*y) + (4*t^8.934)/(g1^12*y) + (3*t^8.956)/(g1^8*y) + (3*t^8.978)/(g1^4*y) - g1*t^4.506*y - (t^7.45*y)/g1^9 - (t^7.494*y)/g1 + g1^3*t^7.517*y + g1^11*t^7.561*y + (2*t^8.867*y)/g1^24 + (2*t^8.89*y)/g1^20 + (4*t^8.912*y)/g1^16 + (4*t^8.934*y)/g1^12 + (3*t^8.956*y)/g1^8 + (3*t^8.978*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 55506 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}M_{6}$ | 0.6918 | 0.8495 | 0.8143 | [M:[1.0137, 0.9973, 0.9863, 1.0082, 0.9918, 0.9863], q:[0.5041, 0.4822], qb:[0.4986, 0.5096], phi:[0.5014]] | t^2.942 + 2*t^2.959 + t^2.975 + t^2.992 + t^3.008 + t^3.025 + t^4.397 + t^4.446 + t^4.463 + t^4.479 + t^4.496 + t^4.512 + 2*t^4.529 + t^4.545 + t^4.562 + t^5.885 + 2*t^5.901 + 3*t^5.918 + 2*t^5.934 + 3*t^5.951 + 3*t^5.967 + t^5.984 - 2*t^6. - t^4.504/y - t^4.504*y | detail |