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 |
|---|---|---|---|---|---|---|---|---|---|
| 57040 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6596 | 0.8201 | 0.8043 | [M:[1.1354, 0.7434, 0.8646, 0.8646, 0.703, 0.8646, 1.2162], q:[0.4929, 0.3717], qb:[0.7636, 0.804], phi:[0.3919]] | [M:[[-16], [-14], [16], [16], [-24], [16], [4]], q:[[23], [-7]], qb:[[-9], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{6}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{7}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{7}$, ${ }M_{5}\phi_{1}q_{1}q_{2}$ | ${}$ | -3 | t^2.109 + t^2.23 + 3*t^2.594 + t^3.527 + t^3.648 + t^3.77 + t^4.133 + t^4.218 + t^4.339 + t^4.461 + t^4.582 + 4*t^4.703 + 2*t^4.824 + t^4.945 + 5*t^5.188 + 3*t^5.758 + t^5.879 - 3*t^6. + 2*t^6.121 + 3*t^6.242 + t^6.327 + 2*t^6.364 + t^6.448 + t^6.57 + 2*t^6.691 + 3*t^6.727 + 3*t^6.812 + 2*t^6.933 + 2*t^7.055 + t^7.176 + 7*t^7.297 + 3*t^7.418 + t^7.539 + 7*t^7.782 + 2*t^7.867 + t^7.903 + 2*t^7.988 - 3*t^8.109 - 2*t^8.23 + t^8.267 + 5*t^8.352 + t^8.436 + t^8.473 + t^8.558 - 9*t^8.594 + t^8.679 + 3*t^8.715 + 2*t^8.8 + 5*t^8.836 + 4*t^8.921 + 2*t^8.958 - t^4.176/y - t^6.285/y - t^6.406/y - (2*t^6.77)/y + t^7.339/y + (2*t^7.582)/y + (3*t^7.703)/y + (3*t^7.824)/y + t^7.945/y + t^8.067/y + (3*t^8.188)/y - t^8.394/y - t^8.515/y + (2*t^8.758)/y - t^4.176*y - t^6.285*y - t^6.406*y - 2*t^6.77*y + t^7.339*y + 2*t^7.582*y + 3*t^7.703*y + 3*t^7.824*y + t^7.945*y + t^8.067*y + 3*t^8.188*y - t^8.394*y - t^8.515*y + 2*t^8.758*y | t^2.109/g1^24 + t^2.23/g1^14 + 3*g1^16*t^2.594 + t^3.527/g1^6 + g1^4*t^3.648 + g1^14*t^3.77 + g1^44*t^4.133 + t^4.218/g1^48 + t^4.339/g1^38 + t^4.461/g1^28 + t^4.582/g1^18 + (4*t^4.703)/g1^8 + 2*g1^2*t^4.824 + g1^12*t^4.945 + 5*g1^32*t^5.188 + (3*t^5.758)/g1^20 + t^5.879/g1^10 - 3*t^6. + 2*g1^10*t^6.121 + 3*g1^20*t^6.242 + t^6.327/g1^72 + 2*g1^30*t^6.364 + t^6.448/g1^62 + t^6.57/g1^52 + (2*t^6.691)/g1^42 + 3*g1^60*t^6.727 + (3*t^6.812)/g1^32 + (2*t^6.933)/g1^22 + (2*t^7.055)/g1^12 + t^7.176/g1^2 + 7*g1^8*t^7.297 + 3*g1^18*t^7.418 + g1^28*t^7.539 + 7*g1^48*t^7.782 + (2*t^7.867)/g1^44 + g1^58*t^7.903 + (2*t^7.988)/g1^34 - (3*t^8.109)/g1^24 - (2*t^8.23)/g1^14 + g1^88*t^8.267 + (5*t^8.352)/g1^4 + t^8.436/g1^96 + g1^6*t^8.473 + t^8.558/g1^86 - 9*g1^16*t^8.594 + t^8.679/g1^76 + 3*g1^26*t^8.715 + (2*t^8.8)/g1^66 + 5*g1^36*t^8.836 + (4*t^8.921)/g1^56 + 2*g1^46*t^8.958 - t^4.176/(g1^2*y) - t^6.285/(g1^26*y) - t^6.406/(g1^16*y) - (2*g1^14*t^6.77)/y + t^7.339/(g1^38*y) + (2*t^7.582)/(g1^18*y) + (3*t^7.703)/(g1^8*y) + (3*g1^2*t^7.824)/y + (g1^12*t^7.945)/y + (g1^22*t^8.067)/y + (3*g1^32*t^8.188)/y - t^8.394/(g1^50*y) - t^8.515/(g1^40*y) + (2*t^8.758)/(g1^20*y) - (t^4.176*y)/g1^2 - (t^6.285*y)/g1^26 - (t^6.406*y)/g1^16 - 2*g1^14*t^6.77*y + (t^7.339*y)/g1^38 + (2*t^7.582*y)/g1^18 + (3*t^7.703*y)/g1^8 + 3*g1^2*t^7.824*y + g1^12*t^7.945*y + g1^22*t^8.067*y + 3*g1^32*t^8.188*y - (t^8.394*y)/g1^50 - (t^8.515*y)/g1^40 + (2*t^8.758*y)/g1^20 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 55433 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{6}$ | 0.677 | 0.851 | 0.7956 | [M:[1.1331, 0.7415, 0.8669, 0.8669, 0.6997, 0.8669], q:[0.4961, 0.3708], qb:[0.7624, 0.8042], phi:[0.3916]] | t^2.099 + t^2.225 + t^2.35 + 3*t^2.601 + t^3.525 + t^3.775 + t^4.152 + t^4.198 + t^4.324 + 2*t^4.449 + 2*t^4.574 + 5*t^4.7 + 2*t^4.825 + 4*t^4.95 + 5*t^5.201 + 2*t^5.749 + t^5.875 - 3*t^6. - t^4.175/y - t^4.175*y | detail |