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 |
|---|---|---|---|---|---|---|---|---|---|
| 57443 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$ | 1.3938 | 1.632 | 0.8541 | [M:[1.1896], q:[0.4105, 0.3896], qb:[0.4, 0.4], phi:[0.4]] | [M:[[1, 1]], q:[[-1, -2], [1, 0]], qb:[[0, 1], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ 2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 4 | 2*t^2.369 + t^2.4 + t^2.431 + 3*t^3.569 + t^3.6 + 2*t^3.631 + 3*t^4.737 + 5*t^4.769 + 5*t^4.8 + 3*t^4.831 + t^4.832 + t^4.863 + 5*t^5.937 + 6*t^5.969 + 4*t^6. + 3*t^6.031 + t^6.032 + t^6.063 + 5*t^7.106 + 12*t^7.137 + 2*t^7.138 + 3*t^7.168 + 10*t^7.169 + 17*t^7.2 + 6*t^7.231 + 2*t^7.232 + 6*t^7.263 + 2*t^7.294 + 7*t^8.306 + 13*t^8.337 + 3*t^8.338 + 5*t^8.368 + 5*t^8.369 + 13*t^8.4 + 3*t^8.431 + t^8.432 + 6*t^8.463 + t^8.494 - t^4.2/y - t^5.4/y - (2*t^6.569)/y - t^6.6/y - t^6.631/y + t^7.737/y - t^7.769/y + t^7.8/y + (3*t^8.937)/y - t^4.2*y - t^5.4*y - 2*t^6.569*y - t^6.6*y - t^6.631*y + t^7.737*y - t^7.769*y + t^7.8*y + 3*t^8.937*y | 2*g1*g2*t^2.369 + t^2.4 + t^2.431/(g1*g2) + 3*g1*g2*t^3.569 + t^3.6 + (2*t^3.631)/(g1*g2) + 3*g1^2*g2^2*t^4.737 + (g1*t^4.769)/g2^2 + 4*g1*g2*t^4.769 + 3*t^4.8 + 2*g2^3*t^4.8 + (3*t^4.831)/(g1*g2) + t^4.832/(g1*g2^4) + t^4.863/(g1^2*g2^2) + 5*g1^2*g2^2*t^5.937 + (g1*t^5.969)/g2^2 + 5*g1*g2*t^5.969 + 2*t^6. + 2*g2^3*t^6. + (3*t^6.031)/(g1*g2) + t^6.032/(g1*g2^4) + t^6.063/(g1^2*g2^2) + g1^3*t^7.106 + 4*g1^3*g2^3*t^7.106 + 12*g1^2*g2^2*t^7.137 + (2*g1^2*t^7.138)/g2 + 3*g1*g2^4*t^7.168 + (2*g1*t^7.169)/g2^2 + 8*g1*g2*t^7.169 + 10*t^7.2 + t^7.2/g2^3 + 6*g2^3*t^7.2 + (5*t^7.231)/(g1*g2) + (g2^2*t^7.231)/g1 + (2*t^7.232)/(g1*g2^4) + t^7.263/(g1^2*g2^5) + (5*t^7.263)/(g1^2*g2^2) + t^7.294/(g1^3*g2^6) + t^7.294/(g1^3*g2^3) + 7*g1^3*g2^3*t^8.306 + 13*g1^2*g2^2*t^8.337 + (3*g1^2*t^8.338)/g2 + 5*g1*g2^4*t^8.368 + (g1*t^8.369)/g2^2 + 4*g1*g2*t^8.369 + 9*t^8.4 + (2*t^8.4)/g2^3 + 2*g2^3*t^8.4 + (2*t^8.431)/(g1*g2) + (g2^2*t^8.431)/g1 + t^8.432/(g1*g2^4) + t^8.463/(g1^2*g2^5) + (5*t^8.463)/(g1^2*g2^2) + t^8.494/(g1^3*g2^3) - t^4.2/y - t^5.4/y - (2*g1*g2*t^6.569)/y - t^6.6/y - t^6.631/(g1*g2*y) + (g1^2*g2^2*t^7.737)/y - (g1*g2*t^7.769)/y + t^7.8/y + (3*g1^2*g2^2*t^8.937)/y - t^4.2*y - t^5.4*y - 2*g1*g2*t^6.569*y - t^6.6*y - (t^6.631*y)/(g1*g2) + g1^2*g2^2*t^7.737*y - g1*g2*t^7.769*y + t^7.8*y + 3*g1^2*g2^2*t^8.937*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47906 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ | 1.3942 | 1.633 | 0.8537 | [M:[1.1779], q:[0.411, 0.389], qb:[0.411, 0.389], phi:[0.4]] | t^2.334 + 3*t^2.4 + 2*t^3.534 + 3*t^3.6 + t^3.666 + t^4.668 + 4*t^4.734 + 2*t^4.767 + 8*t^4.8 + 2*t^4.833 + t^4.866 + 2*t^5.868 + 7*t^5.934 + 2*t^5.967 + 6*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail |