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 |
|---|---|---|---|---|---|---|---|---|---|
| 724 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ | 0.6596 | 0.817 | 0.8073 | [M:[1.1276, 0.7366, 0.8724, 0.8724, 0.8272], q:[0.8045, 0.5041], qb:[0.3683, 0.7593], phi:[0.3909]] | [M:[[16], [14], [-16], [-16], [-6]], q:[[-1], [-23]], qb:[[7], [9]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}^{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | ${}$ | -1 | t^2.21 + t^2.346 + t^2.481 + 2*t^2.617 + t^3.383 + t^3.79 + t^3.926 + t^4.198 + t^4.42 + 2*t^4.556 + 3*t^4.691 + 2*t^4.827 + 4*t^4.963 + 2*t^5.099 + 2*t^5.235 + 2*t^5.728 - t^6. + t^6.136 + t^6.272 + 2*t^6.407 + 3*t^6.543 + t^6.63 + t^6.679 + t^6.765 + 2*t^6.815 + 3*t^6.901 + 3*t^7.037 + 4*t^7.173 + 5*t^7.309 + 4*t^7.444 + 5*t^7.58 + 2*t^7.716 + 2*t^7.852 + t^7.938 + t^7.988 + t^8.074 + t^8.124 - 3*t^8.21 - t^8.346 + t^8.395 - 2*t^8.481 - 3*t^8.617 + 2*t^8.753 + t^8.839 + 4*t^8.889 + t^8.975 - t^4.173/y - t^6.383/y - t^6.519/y - t^6.654/y - t^6.79/y + (2*t^7.556)/y + (2*t^7.691)/y + (4*t^7.827)/y + (3*t^7.963)/y + (2*t^8.099)/y + t^8.235/y - t^8.864/y - t^4.173*y - t^6.383*y - t^6.519*y - t^6.654*y - t^6.79*y + 2*t^7.556*y + 2*t^7.691*y + 4*t^7.827*y + 3*t^7.963*y + 2*t^8.099*y + t^8.235*y - t^8.864*y | g1^14*t^2.21 + g1^4*t^2.346 + t^2.481/g1^6 + (2*t^2.617)/g1^16 + g1^16*t^3.383 + t^3.79/g1^14 + t^3.926/g1^24 + t^4.198/g1^44 + g1^28*t^4.42 + 2*g1^18*t^4.556 + 3*g1^8*t^4.691 + (2*t^4.827)/g1^2 + (4*t^4.963)/g1^12 + (2*t^5.099)/g1^22 + (2*t^5.235)/g1^32 + 2*g1^20*t^5.728 - t^6. + t^6.136/g1^10 + t^6.272/g1^20 + (2*t^6.407)/g1^30 + (3*t^6.543)/g1^40 + g1^42*t^6.63 + t^6.679/g1^50 + g1^32*t^6.765 + (2*t^6.815)/g1^60 + 3*g1^22*t^6.901 + 3*g1^12*t^7.037 + 4*g1^2*t^7.173 + (5*t^7.309)/g1^8 + (4*t^7.444)/g1^18 + (5*t^7.58)/g1^28 + (2*t^7.716)/g1^38 + (2*t^7.852)/g1^48 + g1^34*t^7.938 + t^7.988/g1^58 + g1^24*t^8.074 + t^8.124/g1^68 - 3*g1^14*t^8.21 - g1^4*t^8.346 + t^8.395/g1^88 - (2*t^8.481)/g1^6 - (3*t^8.617)/g1^16 + (2*t^8.753)/g1^26 + g1^56*t^8.839 + (4*t^8.889)/g1^36 + g1^46*t^8.975 - (g1^2*t^4.173)/y - (g1^16*t^6.383)/y - (g1^6*t^6.519)/y - t^6.654/(g1^4*y) - t^6.79/(g1^14*y) + (2*g1^18*t^7.556)/y + (2*g1^8*t^7.691)/y + (4*t^7.827)/(g1^2*y) + (3*t^7.963)/(g1^12*y) + (2*t^8.099)/(g1^22*y) + t^8.235/(g1^32*y) - (g1^10*t^8.864)/y - g1^2*t^4.173*y - g1^16*t^6.383*y - g1^6*t^6.519*y - (t^6.654*y)/g1^4 - (t^6.79*y)/g1^14 + 2*g1^18*t^7.556*y + 2*g1^8*t^7.691*y + (4*t^7.827*y)/g1^2 + (3*t^7.963*y)/g1^12 + (2*t^8.099*y)/g1^22 + (t^8.235*y)/g1^32 - g1^10*t^8.864*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 |
|---|---|---|---|---|---|---|---|---|
| 1191 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{3}M_{6}$ | 0.649 | 0.7983 | 0.813 | [M:[1.1097, 0.721, 0.8903, 0.8903, 0.8339, 1.1097], q:[0.8056, 0.5298], qb:[0.3605, 0.7492], phi:[0.3887]] | t^2.163 + t^2.332 + t^2.502 + t^2.671 + 2*t^3.329 + t^3.837 + t^4.006 + t^4.326 + t^4.345 + 2*t^4.495 + 3*t^4.665 + t^4.834 + 3*t^5.003 + t^5.172 + t^5.492 + 3*t^5.661 + t^5.831 - t^6. - t^4.166/y - t^4.166*y | detail | |
| 1190 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6793 | 0.8531 | 0.7963 | [M:[1.1215, 0.7313, 0.8785, 0.8785, 0.8294, 0.7313], q:[0.8049, 0.5128], qb:[0.3657, 0.7558], phi:[0.3902]] | 2*t^2.194 + t^2.341 + t^2.488 + 2*t^2.636 + t^3.364 + t^3.953 + t^4.248 + 3*t^4.388 + 3*t^4.535 + 4*t^4.682 + 4*t^4.829 + 4*t^4.977 + 2*t^5.124 + 2*t^5.271 + t^5.558 + 2*t^5.706 - 2*t^6. - t^4.171/y - t^4.171*y | detail | |
| 1189 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}^{2}$ | 0.6421 | 0.7861 | 0.8168 | [M:[1.1304, 0.7391, 0.8696, 0.8696, 0.8261, 1.2174], q:[0.8044, 0.5001], qb:[0.3695, 0.7608], phi:[0.3913]] | t^2.217 + t^2.478 + 2*t^2.609 + t^3.391 + t^3.652 + t^3.783 + t^3.913 + t^4.174 + t^4.434 + t^4.565 + 2*t^4.696 + t^4.826 + 2*t^4.957 + 2*t^5.087 + 2*t^5.218 + t^5.739 + t^5.869 - t^6. - t^4.174/y - t^4.174*y | detail | |
| 1192 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{1}q_{2}$ | 0.6803 | 0.8571 | 0.7938 | [M:[1.1242, 0.7337, 0.8758, 0.8758, 0.8284, 0.6863], q:[0.8047, 0.509], qb:[0.3668, 0.7574], phi:[0.3905]] | t^2.059 + t^2.201 + t^2.343 + t^2.485 + 2*t^2.627 + t^3.373 + t^3.799 + t^4.118 + t^4.225 + t^4.26 + 2*t^4.402 + 3*t^4.544 + 5*t^4.686 + 2*t^4.828 + 4*t^4.971 + 2*t^5.113 + 2*t^5.255 + t^5.431 + 2*t^5.716 + t^5.858 - t^6. - t^4.172/y - t^4.172*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 435 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ | 0.645 | 0.7913 | 0.8151 | [M:[1.1221, 0.7318, 0.8779, 0.8779], q:[0.8049, 0.512], qb:[0.3659, 0.7562], phi:[0.3903]] | t^2.195 + t^2.342 + 2*t^2.634 + t^3.366 + t^3.512 + t^3.805 + t^3.951 + t^4.243 + t^4.391 + 2*t^4.537 + 2*t^4.683 + t^4.829 + 3*t^4.975 + 2*t^5.267 + 3*t^5.708 - t^6. - t^4.171/y - t^4.171*y | detail |