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 |
|---|---|---|---|---|---|---|---|---|---|
| 58443 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$ + ${ }q_{2}\tilde{q}_{1}X_{1}$ | 1.1616 | 1.3878 | 0.837 | [X:[1.6], M:[0.7804], q:[0.6798, 0.2601], qb:[0.1399, 0.5202], phi:[0.4]] | [X:[[0]], M:[[3]], q:[[-2], [1]], qb:[[-1], [2]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ 2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ 2}\phi_{1}^{3}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}^{3}\tilde{q}_{2}$ | 6 | 2*t^2.34 + 2*t^2.4 + t^2.46 + t^3.54 + 4*t^3.6 + 3*t^4.68 + 5*t^4.74 + 9*t^4.8 + 3*t^4.86 + t^4.92 + 2*t^5.88 + 10*t^5.94 + 6*t^6. + 4*t^6.06 + 4*t^7.02 + 9*t^7.08 + 18*t^7.14 + 20*t^7.2 + 6*t^7.26 + 3*t^7.32 + t^7.38 + 3*t^8.22 + 17*t^8.28 + 16*t^8.34 + 17*t^8.4 + 3*t^8.46 + 4*t^8.52 - t^4.2/y - t^5.4/y - (2*t^6.54)/y - t^6.6/y - t^6.66/y + t^7.68/y + (2*t^7.74)/y + (2*t^7.86)/y - t^8.88/y + (8*t^8.94)/y - t^4.2*y - t^5.4*y - 2*t^6.54*y - t^6.6*y - t^6.66*y + t^7.68*y + 2*t^7.74*y + 2*t^7.86*y - t^8.88*y + 8*t^8.94*y | 2*g1^3*t^2.34 + 2*t^2.4 + t^2.46/g1^3 + g1^3*t^3.54 + 4*t^3.6 + 3*g1^6*t^4.68 + 5*g1^3*t^4.74 + 9*t^4.8 + (3*t^4.86)/g1^3 + t^4.92/g1^6 + 2*g1^6*t^5.88 + 10*g1^3*t^5.94 + 6*t^6. + (4*t^6.06)/g1^3 + 4*g1^9*t^7.02 + 9*g1^6*t^7.08 + 18*g1^3*t^7.14 + 20*t^7.2 + (6*t^7.26)/g1^3 + (3*t^7.32)/g1^6 + t^7.38/g1^9 + 3*g1^9*t^8.22 + 17*g1^6*t^8.28 + 16*g1^3*t^8.34 + 17*t^8.4 + (3*t^8.46)/g1^3 + (4*t^8.52)/g1^6 - t^4.2/y - t^5.4/y - (2*g1^3*t^6.54)/y - t^6.6/y - t^6.66/(g1^3*y) + (g1^6*t^7.68)/y + (2*g1^3*t^7.74)/y + (2*t^7.86)/(g1^3*y) - (g1^6*t^8.88)/y + (8*g1^3*t^8.94)/y - t^4.2*y - t^5.4*y - 2*g1^3*t^6.54*y - t^6.6*y - (t^6.66*y)/g1^3 + g1^6*t^7.68*y + 2*g1^3*t^7.74*y + (2*t^7.86*y)/g1^3 - g1^6*t^8.88*y + 8*g1^3*t^8.94*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57351 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ | 1.427 | 1.6905 | 0.8441 | [M:[0.7838], q:[0.4098, 0.3951], qb:[0.4065, 0.3887], phi:[0.4]] | 2*t^2.351 + t^2.395 + t^2.4 + t^2.405 + t^2.449 + t^3.551 + t^3.595 + t^3.6 + t^3.605 + 3*t^4.703 + 2*t^4.747 + 4*t^4.751 + 2*t^4.756 + t^4.791 + 2*t^4.795 + 5*t^4.8 + 3*t^4.805 + t^4.809 + 2*t^4.844 + 2*t^4.849 + t^4.853 + t^4.897 + 2*t^5.903 + 2*t^5.947 + 4*t^5.951 + 2*t^5.956 + t^5.991 + 2*t^5.995 + t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail |