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 |
|---|---|---|---|---|---|---|---|---|---|
| 6364 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}M_{7}$ + ${ }M_{3}M_{8}$ + ${ }M_{6}M_{8}$ + ${ }M_{4}M_{9}$ | 0.6598 | 0.8251 | 0.7997 | [M:[0.8894, 0.7106, 0.7553, 0.8447, 1.1553, 0.7553, 0.8447, 1.2447, 1.1553], q:[0.7553, 0.3553], qb:[0.4894, 0.8], phi:[0.4]] | [M:[[2], [-2], [-1], [1], [-1], [-1], [1], [1], [-1]], q:[[-1], [-1]], qb:[[2], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{7}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{9}$, ${ }M_{8}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{6}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{7}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{9}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{6}M_{9}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{2}M_{8}$, ${ }M_{9}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | ${}M_{7}M_{9}$ | -1 | t^2.132 + t^2.266 + t^2.4 + t^2.534 + t^2.668 + t^3.332 + t^3.466 + t^3.734 + t^4.136 + t^4.264 + t^4.398 + 3*t^4.532 + 3*t^4.666 + 2*t^4.8 + 3*t^4.934 + 2*t^5.068 + t^5.336 + t^5.464 + t^5.598 + 3*t^5.732 + 2*t^5.866 - t^6. + t^6.134 + t^6.268 + t^6.395 + t^6.529 + t^6.536 + 4*t^6.664 + t^6.671 + 4*t^6.798 + t^6.805 + 4*t^6.932 + 5*t^7.066 + 3*t^7.2 + 2*t^7.334 + 4*t^7.468 + t^7.595 + 2*t^7.602 + t^7.729 + 4*t^7.864 + t^7.871 + 4*t^7.998 + t^8.005 + t^8.273 + t^8.527 - 3*t^8.534 + t^8.661 - t^8.668 + 4*t^8.795 + t^8.802 + 4*t^8.929 - t^4.2/y - t^6.332/y - t^6.466/y - t^6.6/y - t^6.868/y + t^7.398/y + (2*t^7.532)/y + (2*t^7.666)/y + (3*t^7.8)/y + (3*t^7.934)/y + (2*t^8.068)/y + t^8.202/y + t^8.598/y + (2*t^8.866)/y - t^4.2*y - t^6.332*y - t^6.466*y - t^6.6*y - t^6.868*y + t^7.398*y + 2*t^7.532*y + 2*t^7.666*y + 3*t^7.8*y + 3*t^7.934*y + 2*t^8.068*y + t^8.202*y + t^8.598*y + 2*t^8.866*y | t^2.132/g1^2 + t^2.266/g1 + t^2.4 + g1*t^2.534 + g1^2*t^2.668 + t^3.332/g1^2 + t^3.466/g1 + g1*t^3.734 + g1^4*t^4.136 + t^4.264/g1^4 + t^4.398/g1^3 + (3*t^4.532)/g1^2 + (3*t^4.666)/g1 + 2*t^4.8 + 3*g1*t^4.934 + 2*g1^2*t^5.068 + g1^4*t^5.336 + t^5.464/g1^4 + t^5.598/g1^3 + (3*t^5.732)/g1^2 + (2*t^5.866)/g1 - t^6. + g1*t^6.134 + g1^2*t^6.268 + t^6.395/g1^6 + t^6.529/g1^5 + g1^4*t^6.536 + (4*t^6.664)/g1^4 + g1^5*t^6.671 + (4*t^6.798)/g1^3 + g1^6*t^6.805 + (4*t^6.932)/g1^2 + (5*t^7.066)/g1 + 3*t^7.2 + 2*g1*t^7.334 + 4*g1^2*t^7.468 + t^7.595/g1^6 + 2*g1^3*t^7.602 + t^7.729/g1^5 + (4*t^7.864)/g1^4 + g1^5*t^7.871 + (4*t^7.998)/g1^3 + g1^6*t^8.005 + g1^8*t^8.273 + t^8.527/g1^8 - 3*g1*t^8.534 + t^8.661/g1^7 - g1^2*t^8.668 + (4*t^8.795)/g1^6 + g1^3*t^8.802 + (4*t^8.929)/g1^5 - t^4.2/y - t^6.332/(g1^2*y) - t^6.466/(g1*y) - t^6.6/y - (g1^2*t^6.868)/y + t^7.398/(g1^3*y) + (2*t^7.532)/(g1^2*y) + (2*t^7.666)/(g1*y) + (3*t^7.8)/y + (3*g1*t^7.934)/y + (2*g1^2*t^8.068)/y + (g1^3*t^8.202)/y + t^8.598/(g1^3*y) + (2*t^8.866)/(g1*y) - t^4.2*y - (t^6.332*y)/g1^2 - (t^6.466*y)/g1 - t^6.6*y - g1^2*t^6.868*y + (t^7.398*y)/g1^3 + (2*t^7.532*y)/g1^2 + (2*t^7.666*y)/g1 + 3*t^7.8*y + 3*g1*t^7.934*y + 2*g1^2*t^8.068*y + g1^3*t^8.202*y + (t^8.598*y)/g1^3 + (2*t^8.866*y)/g1 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 4759 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}M_{7}$ + ${ }M_{3}M_{8}$ + ${ }M_{6}M_{8}$ | 0.6735 | 0.8485 | 0.7937 | [M:[0.8784, 0.7216, 0.7608, 0.8392, 1.1608, 0.7608, 0.8392, 1.2392], q:[0.7608, 0.3608], qb:[0.4784, 0.8], phi:[0.4]] | t^2.165 + t^2.282 + t^2.4 + 2*t^2.518 + t^2.635 + t^3.365 + t^3.718 + t^4.07 + t^4.33 + t^4.447 + 3*t^4.565 + 4*t^4.682 + 3*t^4.8 + 4*t^4.918 + 4*t^5.035 + t^5.153 + t^5.27 + t^5.53 + 2*t^5.765 + 2*t^5.882 - 2*t^6. - t^4.2/y - t^4.2*y | detail |