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 |
|---|---|---|---|---|---|---|---|---|---|
| 57979 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | 1.4515 | 1.63 | 0.8904 | [X:[1.3809], M:[0.9134, 0.944], q:[0.518, 0.5027], qb:[0.5686, 0.5533], phi:[0.3096]] | [X:[[0, 4]], M:[[3, -7], [-3, -5]], q:[[-2, 6], [1, 5]], qb:[[-1, 1], [2, 0]], phi:[[0, -2]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }\phi_{1}^{3}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{6}$, ${ }M_{2}\phi_{1}^{3}$, ${ }M_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{3}q_{2}\tilde{q}_{1}$ | -1 | t^2.74 + t^2.79 + t^2.83 + 2*t^3.21 + t^4.1 + 3*t^4.14 + t^4.19 + t^5.03 + 2*t^5.07 + t^5.12 + t^5.48 + t^5.5 + t^5.53 + t^5.55 + 2*t^5.57 + t^5.62 + t^5.66 + t^5.95 - t^6. + 4*t^6.43 + t^6.47 + t^6.84 + 3*t^6.88 + 3*t^6.93 + 2*t^6.97 + t^7.02 + 3*t^7.31 + 6*t^7.36 + 2*t^7.4 + t^7.45 + 2*t^7.77 + t^7.81 + 2*t^7.86 + 2*t^7.9 + t^7.95 + t^8.19 + t^8.22 + 4*t^8.24 + t^8.27 + 7*t^8.29 + 2*t^8.31 + 3*t^8.33 + 2*t^8.36 + t^8.38 + 2*t^8.4 + t^8.45 + t^8.5 + 2*t^8.71 - 4*t^8.74 + 2*t^8.76 - 2*t^8.79 - 3*t^8.83 + t^8.79/y^2 - t^3.93/y - t^4.86/y - t^6.67/y - t^6.71/y - t^6.76/y - (2*t^7.14)/y - t^7.6/y - t^7.64/y - t^7.69/y - (2*t^8.07)/y + t^8.53/y + t^8.57/y + t^8.62/y + t^8.95/y - t^3.93*y - t^4.86*y - t^6.67*y - t^6.71*y - t^6.76*y - 2*t^7.14*y - t^7.6*y - t^7.64*y - t^7.69*y - 2*t^8.07*y + t^8.53*y + t^8.57*y + t^8.62*y + t^8.95*y + t^8.79*y^2 | (g1^3*t^2.74)/g2^7 + t^2.79/g2^6 + t^2.83/(g1^3*g2^5) + 2*g2^6*t^3.21 + g1^3*g2^3*t^4.1 + 3*g2^4*t^4.14 + (g2^5*t^4.19)/g1^3 + g1^3*g2*t^5.03 + 2*g2^2*t^5.07 + (g2^3*t^5.12)/g1^3 + (g1^6*t^5.48)/g2^14 + g2^14*t^5.5 + (g1^3*t^5.53)/g2^13 + (g2^15*t^5.55)/g1^3 + (2*t^5.57)/g2^12 + t^5.62/(g1^3*g2^11) + t^5.66/(g1^6*g2^10) + (g1^3*t^5.95)/g2 - t^6. + 4*g2^12*t^6.43 + (g2^13*t^6.47)/g1^3 + (g1^6*t^6.84)/g2^4 + (3*g1^3*t^6.88)/g2^3 + (3*t^6.93)/g2^2 + (2*t^6.97)/(g1^3*g2) + t^7.02/g1^6 + 3*g1^3*g2^9*t^7.31 + 6*g2^10*t^7.36 + (2*g2^11*t^7.4)/g1^3 + (g2^12*t^7.45)/g1^6 + (2*g1^6*t^7.77)/g2^6 + (g1^3*t^7.81)/g2^5 + (2*t^7.86)/g2^4 + (2*t^7.9)/(g1^3*g2^3) + t^7.95/(g1^6*g2^2) + g1^6*g2^6*t^8.19 + (g1^9*t^8.22)/g2^21 + 4*g1^3*g2^7*t^8.24 + (g1^6*t^8.27)/g2^20 + 7*g2^8*t^8.29 + (2*g1^3*t^8.31)/g2^19 + (3*g2^9*t^8.33)/g1^3 + (2*t^8.36)/g2^18 + (g2^10*t^8.38)/g1^6 + (2*t^8.4)/(g1^3*g2^17) + t^8.45/(g1^6*g2^16) + t^8.5/(g1^9*g2^15) + 2*g2^20*t^8.71 - (4*g1^3*t^8.74)/g2^7 + (2*g2^21*t^8.76)/g1^3 - (2*t^8.79)/g2^6 - (3*t^8.83)/(g1^3*g2^5) + t^8.79/(g2^6*y^2) - t^3.93/(g2^2*y) - t^4.86/(g2^4*y) - (g1^3*t^6.67)/(g2^9*y) - t^6.71/(g2^8*y) - t^6.76/(g1^3*g2^7*y) - (2*g2^4*t^7.14)/y - (g1^3*t^7.6)/(g2^11*y) - t^7.64/(g2^10*y) - t^7.69/(g1^3*g2^9*y) - (2*g2^2*t^8.07)/y + (g1^3*t^8.53)/(g2^13*y) + t^8.57/(g2^12*y) + t^8.62/(g1^3*g2^11*y) + (g1^3*t^8.95)/(g2*y) - (t^3.93*y)/g2^2 - (t^4.86*y)/g2^4 - (g1^3*t^6.67*y)/g2^9 - (t^6.71*y)/g2^8 - (t^6.76*y)/(g1^3*g2^7) - 2*g2^4*t^7.14*y - (g1^3*t^7.6*y)/g2^11 - (t^7.64*y)/g2^10 - (t^7.69*y)/(g1^3*g2^9) - 2*g2^2*t^8.07*y + (g1^3*t^8.53*y)/g2^13 + (t^8.57*y)/g2^12 + (t^8.62*y)/(g1^3*g2^11) + (g1^3*t^8.95*y)/g2 + (t^8.79*y^2)/g2^6 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 57307 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.4518 | 1.6306 | 0.8903 | [X:[1.3795], M:[0.9159, 0.9457], q:[0.5105, 0.5119], qb:[0.5736, 0.5425], phi:[0.3103]] | t^2.748 + t^2.792 + t^2.837 + t^3.159 + t^3.256 + t^4.09 + t^4.094 + t^4.138 + t^4.183 + t^4.187 + t^5.02 + t^5.025 + t^5.114 + t^5.118 + t^5.495 + t^5.529 + t^5.533 + t^5.54 + 2*t^5.585 + t^5.629 + t^5.674 + t^5.906 + t^5.951 - 3*t^6. - t^3.931/y - t^4.862/y - t^3.931*y - t^4.862*y | detail |