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 |
|---|---|---|---|---|---|---|---|---|---|
| 4599 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{4}M_{7}$ + ${ }M_{6}M_{8}$ | 0.699 | 0.8609 | 0.8119 | [M:[0.9154, 1.0604, 0.9396, 1.0363, 0.9637, 1.0121, 0.9637, 0.9879], q:[0.5544, 0.5302], qb:[0.506, 0.4335], phi:[0.494]] | [M:[[14], [-10], [10], [-6], [6], [-2], [6], [2]], q:[[-9], [-5]], qb:[[-1], [11]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{7}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{7}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{7}$, ${ }M_{1}M_{8}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{3}M_{8}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{8}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$ | ${}$ | -3 | t^2.746 + t^2.819 + 2*t^2.891 + 2*t^2.964 + t^3.181 + t^4.083 + t^4.301 + t^4.373 + t^4.446 + t^4.518 + t^4.591 + 2*t^4.663 + t^4.736 + t^4.808 + t^5.492 + t^5.565 + 2*t^5.637 + 3*t^5.71 + 4*t^5.782 + 3*t^5.855 + 2*t^5.927 - 3*t^6. - t^6.073 + t^6.145 - t^6.218 - t^6.29 + t^6.829 + t^6.902 + 2*t^6.974 + 3*t^7.047 + 2*t^7.192 + 5*t^7.264 + 3*t^7.337 + 3*t^7.409 + 2*t^7.482 + 3*t^7.554 + 4*t^7.627 + t^7.699 - t^7.844 + t^7.989 + t^8.166 + t^8.239 + t^8.311 + 3*t^8.384 + 4*t^8.456 + 4*t^8.529 + 4*t^8.601 + 7*t^8.674 + 4*t^8.746 - 4*t^8.891 - 8*t^8.964 - t^4.482/y - t^7.228/y - t^7.373/y - t^7.446/y + t^7.518/y + t^7.591/y + t^7.736/y + t^8.565/y + (2*t^8.637)/y + (4*t^8.71)/y + (3*t^8.782)/y + (4*t^8.855)/y + (2*t^8.927)/y - t^4.482*y - t^7.228*y - t^7.373*y - t^7.446*y + t^7.518*y + t^7.591*y + t^7.736*y + t^8.565*y + 2*t^8.637*y + 4*t^8.71*y + 3*t^8.782*y + 4*t^8.855*y + 2*t^8.927*y | g1^14*t^2.746 + g1^10*t^2.819 + 2*g1^6*t^2.891 + 2*g1^2*t^2.964 + t^3.181/g1^10 + g1^23*t^4.083 + g1^11*t^4.301 + g1^7*t^4.373 + g1^3*t^4.446 + t^4.518/g1 + t^4.591/g1^5 + (2*t^4.663)/g1^9 + t^4.736/g1^13 + t^4.808/g1^17 + g1^28*t^5.492 + g1^24*t^5.565 + 2*g1^20*t^5.637 + 3*g1^16*t^5.71 + 4*g1^12*t^5.782 + 3*g1^8*t^5.855 + 2*g1^4*t^5.927 - 3*t^6. - t^6.073/g1^4 + t^6.145/g1^8 - t^6.218/g1^12 - t^6.29/g1^16 + g1^37*t^6.829 + g1^33*t^6.902 + 2*g1^29*t^6.974 + 3*g1^25*t^7.047 + 2*g1^17*t^7.192 + 5*g1^13*t^7.264 + 3*g1^9*t^7.337 + 3*g1^5*t^7.409 + 2*g1*t^7.482 + (3*t^7.554)/g1^3 + (4*t^7.627)/g1^7 + t^7.699/g1^11 - t^7.844/g1^19 + t^7.989/g1^27 + g1^46*t^8.166 + g1^42*t^8.239 + g1^38*t^8.311 + 3*g1^34*t^8.384 + 4*g1^30*t^8.456 + 4*g1^26*t^8.529 + 4*g1^22*t^8.601 + 7*g1^18*t^8.674 + 4*g1^14*t^8.746 - 4*g1^6*t^8.891 - 8*g1^2*t^8.964 - (g1*t^4.482)/y - (g1^15*t^7.228)/y - (g1^7*t^7.373)/y - (g1^3*t^7.446)/y + t^7.518/(g1*y) + t^7.591/(g1^5*y) + t^7.736/(g1^13*y) + (g1^24*t^8.565)/y + (2*g1^20*t^8.637)/y + (4*g1^16*t^8.71)/y + (3*g1^12*t^8.782)/y + (4*g1^8*t^8.855)/y + (2*g1^4*t^8.927)/y - g1*t^4.482*y - g1^15*t^7.228*y - g1^7*t^7.373*y - g1^3*t^7.446*y + (t^7.518*y)/g1 + (t^7.591*y)/g1^5 + (t^7.736*y)/g1^13 + g1^24*t^8.565*y + 2*g1^20*t^8.637*y + 4*g1^16*t^8.71*y + 3*g1^12*t^8.782*y + 4*g1^8*t^8.855*y + 2*g1^4*t^8.927*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2545 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{4}M_{7}$ | 0.6979 | 0.8587 | 0.8127 | [M:[0.9216, 1.056, 0.944, 1.0336, 0.9664, 1.0112, 0.9664], q:[0.5504, 0.528], qb:[0.5056, 0.4384], phi:[0.4944]] | t^2.765 + t^2.832 + 2*t^2.899 + t^2.966 + t^3.034 + t^3.168 + t^4.113 + t^4.315 + t^4.382 + t^4.45 + t^4.517 + t^4.584 + 2*t^4.651 + t^4.719 + t^4.786 + t^5.529 + t^5.597 + 2*t^5.664 + 2*t^5.731 + 4*t^5.798 + 2*t^5.866 + 2*t^5.933 - 2*t^6. - t^4.483/y - t^4.483*y | detail |