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 |
|---|---|---|---|---|---|---|---|---|---|
| 1656 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{2}^{2}$ | 0.7228 | 0.9222 | 0.7838 | [M:[0.9709, 1.124, 0.9709, 0.6861, 0.876, 0.6861, 0.6861], q:[0.781, 0.438], qb:[0.5911, 0.438], phi:[0.438]] | [M:[[9], [-4], [9], [-6], [4], [-6], [-6]], q:[[-1], [2]], qb:[[-11], [2]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{6}$, ${ }M_{7}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{3}$, ${ }q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{7}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{3}M_{7}$, ${ }M_{5}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{6}q_{1}q_{2}$, ${ }M_{7}q_{1}q_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{7}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$ | ${}$ | -5 | 3*t^2.058 + 2*t^2.628 + 2*t^2.913 + 2*t^3.657 + 7*t^4.116 + 2*t^4.401 + 6*t^4.686 + t^4.861 + 6*t^4.971 + 3*t^5.256 + 2*t^5.541 + 6*t^5.715 + 3*t^5.826 - 5*t^6. + 13*t^6.174 + 2*t^6.285 + 4*t^6.459 + 3*t^6.57 + 12*t^6.744 - 2*t^6.855 + 3*t^6.919 + 14*t^7.029 + 9*t^7.314 + t^7.488 + 4*t^7.599 + 12*t^7.773 + 12*t^7.884 - 15*t^8.058 + 2*t^8.169 + 21*t^8.233 + 2*t^8.343 + 3*t^8.453 + 8*t^8.518 - t^8.628 + 4*t^8.738 + 19*t^8.802 - 12*t^8.913 + 7*t^8.977 - t^4.314/y - (3*t^6.372)/y - t^6.942/y + (3*t^7.116)/y - (2*t^7.227)/y + (2*t^7.401)/y + (7*t^7.686)/y + (6*t^7.971)/y + (4*t^8.256)/y - (6*t^8.43)/y + (4*t^8.541)/y + (6*t^8.715)/y + t^8.826/y - t^4.314*y - 3*t^6.372*y - t^6.942*y + 3*t^7.116*y - 2*t^7.227*y + 2*t^7.401*y + 7*t^7.686*y + 6*t^7.971*y + 4*t^8.256*y - 6*t^8.43*y + 4*t^8.541*y + 6*t^8.715*y + t^8.826*y | (3*t^2.058)/g1^6 + 2*g1^4*t^2.628 + 2*g1^9*t^2.913 + 2*g1*t^3.657 + (7*t^4.116)/g1^12 + (2*t^4.401)/g1^7 + (6*t^4.686)/g1^2 + t^4.861/g1^20 + 6*g1^3*t^4.971 + 3*g1^8*t^5.256 + 2*g1^13*t^5.541 + (6*t^5.715)/g1^5 + 3*g1^18*t^5.826 - 5*t^6. + (13*t^6.174)/g1^18 + 2*g1^5*t^6.285 + (4*t^6.459)/g1^13 + 3*g1^10*t^6.57 + (12*t^6.744)/g1^8 - 2*g1^15*t^6.855 + (3*t^6.919)/g1^26 + (14*t^7.029)/g1^3 + 9*g1^2*t^7.314 + t^7.488/g1^16 + 4*g1^7*t^7.599 + (12*t^7.773)/g1^11 + 12*g1^12*t^7.884 - (15*t^8.058)/g1^6 + 2*g1^17*t^8.169 + (21*t^8.233)/g1^24 + (2*t^8.343)/g1 + 3*g1^22*t^8.453 + (8*t^8.518)/g1^19 - g1^4*t^8.628 + 4*g1^27*t^8.738 + (19*t^8.802)/g1^14 - 12*g1^9*t^8.913 + (7*t^8.977)/g1^32 - (g1^2*t^4.314)/y - (3*t^6.372)/(g1^4*y) - (g1^6*t^6.942)/y + (3*t^7.116)/(g1^12*y) - (2*g1^11*t^7.227)/y + (2*t^7.401)/(g1^7*y) + (7*t^7.686)/(g1^2*y) + (6*g1^3*t^7.971)/y + (4*g1^8*t^8.256)/y - (6*t^8.43)/(g1^10*y) + (4*g1^13*t^8.541)/y + (6*t^8.715)/(g1^5*y) + (g1^18*t^8.826)/y - g1^2*t^4.314*y - (3*t^6.372*y)/g1^4 - g1^6*t^6.942*y + (3*t^7.116*y)/g1^12 - 2*g1^11*t^7.227*y + (2*t^7.401*y)/g1^7 + (7*t^7.686*y)/g1^2 + 6*g1^3*t^7.971*y + 4*g1^8*t^8.256*y - (6*t^8.43*y)/g1^10 + 4*g1^13*t^8.541*y + (6*t^8.715*y)/g1^5 + g1^18*t^8.826*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 |
|---|---|---|---|---|---|---|---|---|---|
| 1062 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$ | 0.7021 | 0.8818 | 0.7962 | [M:[0.9685, 1.1251, 0.9685, 0.6876, 0.8749, 0.6876], q:[0.7813, 0.4375], qb:[0.594, 0.4375], phi:[0.4375]] | 2*t^2.063 + 2*t^2.625 + 2*t^2.906 + 2*t^3.656 + t^3.937 + 4*t^4.126 + 2*t^4.407 + 4*t^4.688 + t^4.876 + 4*t^4.969 + 3*t^5.249 + 2*t^5.53 + 4*t^5.719 + 3*t^5.811 - 3*t^6. - t^4.312/y - t^4.312*y | detail |