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 |
|---|---|---|---|---|---|---|---|---|---|
| 57455 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{6}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ | 1.4391 | 1.6266 | 0.8847 | [X:[1.3333], M:[0.9997], q:[0.5335, 0.5666], qb:[0.4668, 0.4331], phi:[0.3333]] | [X:[[0, 0]], M:[[1, 2]], q:[[-2, -2], [1, 1]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.9 + 2*t^2.999 + t^3. + t^3.1 + t^3.9 + t^3.999 + t^4. + t^4.001 + t^4.1 + t^4.9 + 2*t^4.999 + t^5.001 + 2*t^5.1 + t^5.8 + t^5.899 + t^5.9 + 3*t^5.998 + 3*t^5.999 - t^6. + t^6.099 + 2*t^6.1 - t^6.101 + t^6.2 + t^6.8 + t^6.898 + 2*t^6.899 + 2*t^6.9 + t^6.901 + 2*t^6.998 + 4*t^6.999 + 2*t^7. + t^7.001 + t^7.099 + 3*t^7.1 + t^7.2 + t^7.201 + 2*t^7.8 + t^7.802 + 3*t^7.899 + 2*t^7.901 + 4*t^7.998 + 2*t^7.999 + 4*t^8. + t^8.002 + 5*t^8.099 + 2*t^8.1 + 2*t^8.2 + t^8.7 + t^8.799 + 2*t^8.8 - t^8.801 + t^8.898 + 4*t^8.899 - 2*t^8.9 + 2*t^8.901 - t^8.902 + 4*t^8.997 + 6*t^8.998 - 3*t^8.999 - t^4./y - t^5./y - t^6.9/y - (2*t^6.999)/y - t^7./y - t^7.1/y - t^7.9/y - (2*t^7.999)/y - t^8./y - t^8.1/y + (2*t^8.899)/y + t^8.998/y + t^8.999/y - t^4.*y - t^5.*y - t^6.9*y - 2*t^6.999*y - t^7.*y - t^7.1*y - t^7.9*y - 2*t^7.999*y - t^8.*y - t^8.1*y + 2*t^8.899*y + t^8.998*y + t^8.999*y | t^2.9/(g1^2*g2) + 2*g1*g2^2*t^2.999 + t^3. + g1^2*g2*t^3.1 + t^3.9/(g1^2*g2) + g1*g2^2*t^3.999 + t^4. + t^4.001/(g1*g2^2) + g1^2*g2*t^4.1 + t^4.9/(g1^2*g2) + 2*g1*g2^2*t^4.999 + t^5.001/(g1*g2^2) + 2*g1^2*g2*t^5.1 + t^5.8/(g1^4*g2^2) + (g2*t^5.899)/g1 + t^5.9/(g1^2*g2) + 3*g1^2*g2^4*t^5.998 + 3*g1*g2^2*t^5.999 - t^6. + g1^3*g2^3*t^6.099 + 2*g1^2*g2*t^6.1 - (g1*t^6.101)/g2 + g1^4*g2^2*t^6.2 + t^6.8/(g1^4*g2^2) + g2^3*t^6.898 + (2*g2*t^6.899)/g1 + (2*t^6.9)/(g1^2*g2) + t^6.901/(g1^3*g2^3) + 2*g1^2*g2^4*t^6.998 + 4*g1*g2^2*t^6.999 + 2*t^7. + t^7.001/(g1*g2^2) + g1^3*g2^3*t^7.099 + 3*g1^2*g2*t^7.1 + g1^4*g2^2*t^7.2 + g1^3*t^7.201 + (2*t^7.8)/(g1^4*g2^2) + t^7.802/(g1^6*g2^6) + (3*g2*t^7.899)/g1 + (2*t^7.901)/(g1^3*g2^3) + 4*g1^2*g2^4*t^7.998 + 2*g1*g2^2*t^7.999 + 4*t^8. + t^8.002/(g1^2*g2^4) + 5*g1^3*g2^3*t^8.099 + 2*g1^2*g2*t^8.1 + 2*g1^4*g2^2*t^8.2 + t^8.7/(g1^6*g2^3) + t^8.799/g1^3 + (2*t^8.8)/(g1^4*g2^2) - t^8.801/(g1^5*g2^4) + g2^3*t^8.898 + (4*g2*t^8.899)/g1 - (2*t^8.9)/(g1^2*g2) + (2*t^8.901)/(g1^3*g2^3) - t^8.902/(g1^4*g2^5) + 4*g1^3*g2^6*t^8.997 + 6*g1^2*g2^4*t^8.998 - 3*g1*g2^2*t^8.999 - t^4./y - t^5./y - t^6.9/(g1^2*g2*y) - (2*g1*g2^2*t^6.999)/y - t^7./y - (g1^2*g2*t^7.1)/y - t^7.9/(g1^2*g2*y) - (2*g1*g2^2*t^7.999)/y - t^8./y - (g1^2*g2*t^8.1)/y + (2*g2*t^8.899)/(g1*y) + (g1^2*g2^4*t^8.998)/y + (g1*g2^2*t^8.999)/y - t^4.*y - t^5.*y - (t^6.9*y)/(g1^2*g2) - 2*g1*g2^2*t^6.999*y - t^7.*y - g1^2*g2*t^7.1*y - (t^7.9*y)/(g1^2*g2) - 2*g1*g2^2*t^7.999*y - t^8.*y - g1^2*g2*t^8.1*y + (2*g2*t^8.899*y)/g1 + g1^2*g2^4*t^8.998*y + g1*g2^2*t^8.999*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47889 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{6}$ | 1.4548 | 1.6446 | 0.8846 | [X:[1.3333], M:[0.9634], q:[0.5183, 0.4817], qb:[0.5183, 0.4817], phi:[0.3333]] | 2*t^2.89 + 3*t^3. + t^3.89 + 3*t^4. + t^4.11 + t^4.89 + 2*t^5. + t^5.11 + 2*t^5.445 + 2*t^5.555 + 3*t^5.78 + 4*t^5.89 + 2*t^6. - t^4./y - t^5./y - t^4.*y - t^5.*y | detail |