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 |
|---|---|---|---|---|---|---|---|---|---|
| 6113 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{3}M_{7}$ + ${ }M_{4}M_{8}$ + ${ }M_{6}M_{9}$ | 0.6944 | 0.8518 | 0.8152 | [M:[0.9462, 1.0384, 0.9616, 1.023, 0.977, 1.0077, 1.0384, 0.977, 0.9923], q:[0.5346, 0.5192], qb:[0.5038, 0.4578], phi:[0.4962]] | [M:[[14], [-10], [10], [-6], [6], [-2], [-10], [6], [2]], q:[[-9], [-5]], qb:[[-1], [11]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{5}$, ${ }M_{8}$, ${ }M_{9}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{7}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{8}$, ${ }M_{1}M_{9}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{5}M_{9}$, ${ }M_{8}M_{9}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{7}$, ${ }M_{9}^{2}$, ${ }M_{9}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$ | ${}$ | -4 | t^2.839 + 2*t^2.931 + 2*t^2.977 + 2*t^3.115 + t^4.235 + t^4.373 + t^4.419 + t^4.465 + t^4.512 + t^4.558 + 2*t^4.604 + t^4.65 + t^4.696 + t^5.677 + t^5.77 + t^5.816 + 2*t^5.862 + 3*t^5.908 + 3*t^5.954 - 4*t^6. + t^6.046 + 3*t^6.092 - t^6.138 - t^6.184 + 2*t^6.23 + t^7.074 + 2*t^7.166 + 3*t^7.212 - t^7.258 + t^7.304 + 5*t^7.35 + 2*t^7.396 + 2*t^7.442 + t^7.488 + 3*t^7.535 + 4*t^7.581 + 2*t^7.627 + t^7.673 + t^7.719 + t^7.765 + 2*t^7.811 + t^8.47 + t^8.516 + 2*t^8.608 + 2*t^8.654 + t^8.7 + 5*t^8.793 + 2*t^8.839 + 4*t^8.885 - 2*t^8.931 - 7*t^8.977 - t^4.488/y - t^7.327/y + t^7.373/y - t^7.419/y - t^7.465/y + t^7.512/y + t^7.558/y - t^7.604/y + t^7.65/y + (2*t^8.77)/y + (2*t^8.816)/y + t^8.862/y + (4*t^8.908)/y + (3*t^8.954)/y - t^4.488*y - t^7.327*y + t^7.373*y - t^7.419*y - t^7.465*y + t^7.512*y + t^7.558*y - t^7.604*y + t^7.65*y + 2*t^8.77*y + 2*t^8.816*y + t^8.862*y + 4*t^8.908*y + 3*t^8.954*y | g1^14*t^2.839 + 2*g1^6*t^2.931 + 2*g1^2*t^2.977 + (2*t^3.115)/g1^10 + g1^23*t^4.235 + g1^11*t^4.373 + g1^7*t^4.419 + g1^3*t^4.465 + t^4.512/g1 + t^4.558/g1^5 + (2*t^4.604)/g1^9 + t^4.65/g1^13 + t^4.696/g1^17 + g1^28*t^5.677 + g1^20*t^5.77 + g1^16*t^5.816 + 2*g1^12*t^5.862 + 3*g1^8*t^5.908 + 3*g1^4*t^5.954 - 4*t^6. + t^6.046/g1^4 + (3*t^6.092)/g1^8 - t^6.138/g1^12 - t^6.184/g1^16 + (2*t^6.23)/g1^20 + g1^37*t^7.074 + 2*g1^29*t^7.166 + 3*g1^25*t^7.212 - g1^21*t^7.258 + g1^17*t^7.304 + 5*g1^13*t^7.35 + 2*g1^9*t^7.396 + 2*g1^5*t^7.442 + g1*t^7.488 + (3*t^7.535)/g1^3 + (4*t^7.581)/g1^7 + (2*t^7.627)/g1^11 + t^7.673/g1^15 + t^7.719/g1^19 + t^7.765/g1^23 + (2*t^7.811)/g1^27 + g1^46*t^8.47 + g1^42*t^8.516 + 2*g1^34*t^8.608 + 2*g1^30*t^8.654 + g1^26*t^8.7 + 5*g1^18*t^8.793 + 2*g1^14*t^8.839 + 4*g1^10*t^8.885 - 2*g1^6*t^8.931 - 7*g1^2*t^8.977 - (g1*t^4.488)/y - (g1^15*t^7.327)/y + (g1^11*t^7.373)/y - (g1^7*t^7.419)/y - (g1^3*t^7.465)/y + t^7.512/(g1*y) + t^7.558/(g1^5*y) - t^7.604/(g1^9*y) + t^7.65/(g1^13*y) + (2*g1^20*t^8.77)/y + (2*g1^16*t^8.816)/y + (g1^12*t^8.862)/y + (4*g1^8*t^8.908)/y + (3*g1^4*t^8.954)/y - g1*t^4.488*y - g1^15*t^7.327*y + g1^11*t^7.373*y - g1^7*t^7.419*y - g1^3*t^7.465*y + (t^7.512*y)/g1 + (t^7.558*y)/g1^5 - (t^7.604*y)/g1^9 + (t^7.65*y)/g1^13 + 2*g1^20*t^8.77*y + 2*g1^16*t^8.816*y + g1^12*t^8.862*y + 4*g1^8*t^8.908*y + 3*g1^4*t^8.954*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 |
|---|---|---|---|---|---|---|---|---|---|
| 4594 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{3}M_{7}$ + ${ }M_{4}M_{8}$ | 0.6937 | 0.8506 | 0.8156 | [M:[0.9527, 1.0338, 0.9662, 1.0203, 0.9797, 1.0068, 1.0338, 0.9797], q:[0.5304, 0.5169], qb:[0.5034, 0.4628], phi:[0.4966]] | t^2.858 + 2*t^2.939 + t^2.98 + t^3.02 + 2*t^3.101 + t^4.267 + t^4.389 + t^4.429 + t^4.47 + t^4.51 + t^4.551 + 2*t^4.591 + t^4.632 + t^4.672 + t^5.716 + t^5.797 + 3*t^5.878 + t^5.919 + 3*t^5.959 - 3*t^6. - t^4.49/y - t^4.49*y | detail |