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 |
|---|---|---|---|---|---|---|---|---|---|
| 58376 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$ | 1.3408 | 1.58 | 0.8486 | [X:[1.4], M:[0.7724], q:[0.3425, 0.5149], qb:[0.4851, 0.2575], phi:[0.4]] | [X:[[0]], M:[[3]], q:[[-1], [2]], qb:[[-2], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$ | ${2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$ | 2 | 2*t^2.32 + t^2.4 + t^2.48 + 2*t^3. + t^3.52 + t^3.6 + 4*t^4.2 + 3*t^4.63 + 3*t^4.72 + 4*t^4.8 + 3*t^4.88 + t^4.97 + 4*t^5.32 + 4*t^5.4 + t^5.48 + 2*t^5.83 + 4*t^5.92 + 2*t^6. + 2*t^6.08 + 9*t^6.52 + 6*t^6.6 + 2*t^6.68 + 4*t^6.95 + 6*t^7.03 + 7*t^7.12 + 13*t^7.2 + 6*t^7.28 + 3*t^7.37 + t^7.45 + 6*t^7.63 + 12*t^7.72 + 7*t^7.8 + 2*t^7.88 + 2*t^7.97 + 3*t^8.15 + 9*t^8.23 + 3*t^8.32 + 15*t^8.4 + t^8.57 + 13*t^8.83 + 17*t^8.92 - t^4.2/y - t^5.4/y - (2*t^6.52)/y - t^6.6/y - t^6.68/y - t^7.2/y + t^7.63/y + t^7.8/y + t^7.88/y + (4*t^8.32)/y - t^8.4/y + (2*t^8.48)/y - t^8.83/y - t^4.2*y - t^5.4*y - 2*t^6.52*y - t^6.6*y - t^6.68*y - t^7.2*y + t^7.63*y + t^7.8*y + t^7.88*y + 4*t^8.32*y - t^8.4*y + 2*t^8.48*y - t^8.83*y | 2*g1^3*t^2.32 + t^2.4 + t^2.48/g1^3 + 2*t^3. + g1^3*t^3.52 + t^3.6 + 4*t^4.2 + 3*g1^6*t^4.63 + 3*g1^3*t^4.72 + 4*t^4.8 + (3*t^4.88)/g1^3 + t^4.97/g1^6 + 4*g1^3*t^5.32 + 4*t^5.4 + t^5.48/g1^3 + 2*g1^6*t^5.83 + 4*g1^3*t^5.92 + 2*t^6. + (2*t^6.08)/g1^3 + 9*g1^3*t^6.52 + 6*t^6.6 + (2*t^6.68)/g1^3 + 4*g1^9*t^6.95 + 6*g1^6*t^7.03 + 7*g1^3*t^7.12 + 13*t^7.2 + (6*t^7.28)/g1^3 + (3*t^7.37)/g1^6 + t^7.45/g1^9 + 6*g1^6*t^7.63 + 12*g1^3*t^7.72 + 7*t^7.8 + (2*t^7.88)/g1^3 + (2*t^7.97)/g1^6 + 3*g1^9*t^8.15 + 9*g1^6*t^8.23 + 3*g1^3*t^8.32 + 15*t^8.4 + t^8.57/g1^6 + 13*g1^6*t^8.83 + 17*g1^3*t^8.92 - t^4.2/y - t^5.4/y - (2*g1^3*t^6.52)/y - t^6.6/y - t^6.68/(g1^3*y) - t^7.2/y + (g1^6*t^7.63)/y + t^7.8/y + t^7.88/(g1^3*y) + (4*g1^3*t^8.32)/y - t^8.4/y + (2*t^8.48)/(g1^3*y) - (g1^6*t^8.83)/y - t^4.2*y - t^5.4*y - 2*g1^3*t^6.52*y - t^6.6*y - (t^6.68*y)/g1^3 - t^7.2*y + g1^6*t^7.63*y + t^7.8*y + (t^7.88*y)/g1^3 + 4*g1^3*t^8.32*y - t^8.4*y + (2*t^8.48*y)/g1^3 - g1^6*t^8.83*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57346 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ | 1.3468 | 1.5854 | 0.8495 | [X:[1.4], M:[0.7819], q:[0.3076, 0.4894], qb:[0.5106, 0.2924], phi:[0.4]] | 2*t^2.346 + t^2.4 + t^2.454 + 2*t^3. + t^3.546 + t^3.6 + 3*t^4.2 + t^4.486 + t^4.514 + 3*t^4.691 + 3*t^4.746 + 3*t^4.8 + 2*t^4.854 + t^4.909 + t^5.059 + t^5.141 + 3*t^5.346 + 3*t^5.4 + t^5.454 + t^5.686 + t^5.714 + 2*t^5.891 + 3*t^5.946 + t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail |