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 |
|---|---|---|---|---|---|---|---|---|---|
| 58372 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ | 1.2929 | 1.5266 | 0.8469 | [X:[1.4], M:[0.861], q:[0.3594, 0.6203], qb:[0.3797, 0.2406], 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 |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$ | ${2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ | 2 | t^2.22 + t^2.4 + 2*t^2.58 + 2*t^3. + t^3.6 + 2*t^3.78 + 4*t^4.2 + t^4.43 + 2*t^4.62 + 3*t^4.8 + 4*t^4.98 + 3*t^5.17 + 2*t^5.22 + 4*t^5.4 + 3*t^5.58 + t^5.77 + t^5.82 + 2*t^6. + 5*t^6.18 + 4*t^6.37 + 3*t^6.42 + 6*t^6.6 + t^6.65 + 8*t^6.78 + 3*t^6.83 + 4*t^7.02 + 10*t^7.2 + 7*t^7.38 + 2*t^7.43 + 9*t^7.57 + 4*t^7.62 + 4*t^7.75 + 7*t^7.8 + 13*t^7.98 + t^8.03 + 4*t^8.17 + 2*t^8.35 + 14*t^8.4 + 4*t^8.58 + 2*t^8.63 + 13*t^8.77 + 5*t^8.82 + t^8.87 + 6*t^8.95 - t^4.2/y - t^5.4/y - t^6.42/y - t^6.6/y - (2*t^6.78)/y - t^7.2/y + t^7.62/y + t^7.8/y + t^8.17/y + (2*t^8.22)/y - t^8.4/y + (4*t^8.58)/y - t^8.63/y - t^4.2*y - t^5.4*y - t^6.42*y - t^6.6*y - 2*t^6.78*y - t^7.2*y + t^7.62*y + t^7.8*y + t^8.17*y + 2*t^8.22*y - t^8.4*y + 4*t^8.58*y - t^8.63*y | t^2.22/g1^3 + t^2.4 + 2*g1^3*t^2.58 + 2*t^3. + t^3.6 + 2*g1^3*t^3.78 + 4*t^4.2 + t^4.43/g1^6 + (2*t^4.62)/g1^3 + 3*t^4.8 + 4*g1^3*t^4.98 + 3*g1^6*t^5.17 + (2*t^5.22)/g1^3 + 4*t^5.4 + 3*g1^3*t^5.58 + g1^6*t^5.77 + t^5.82/g1^3 + 2*t^6. + 5*g1^3*t^6.18 + 4*g1^6*t^6.37 + (3*t^6.42)/g1^3 + 6*t^6.6 + t^6.65/g1^9 + 8*g1^3*t^6.78 + (3*t^6.83)/g1^6 + (4*t^7.02)/g1^3 + 10*t^7.2 + 7*g1^3*t^7.38 + (2*t^7.43)/g1^6 + 9*g1^6*t^7.57 + (4*t^7.62)/g1^3 + 4*g1^9*t^7.75 + 7*t^7.8 + 13*g1^3*t^7.98 + t^8.03/g1^6 + 4*g1^6*t^8.17 + 2*g1^9*t^8.35 + 14*t^8.4 + 4*g1^3*t^8.58 + (2*t^8.63)/g1^6 + 13*g1^6*t^8.77 + (5*t^8.82)/g1^3 + t^8.87/g1^12 + 6*g1^9*t^8.95 - t^4.2/y - t^5.4/y - t^6.42/(g1^3*y) - t^6.6/y - (2*g1^3*t^6.78)/y - t^7.2/y + t^7.62/(g1^3*y) + t^7.8/y + (g1^6*t^8.17)/y + (2*t^8.22)/(g1^3*y) - t^8.4/y + (4*g1^3*t^8.58)/y - t^8.63/(g1^6*y) - t^4.2*y - t^5.4*y - (t^6.42*y)/g1^3 - t^6.6*y - 2*g1^3*t^6.78*y - t^7.2*y + (t^7.62*y)/g1^3 + t^7.8*y + g1^6*t^8.17*y + (2*t^8.22*y)/g1^3 - t^8.4*y + 4*g1^3*t^8.58*y - (t^8.63*y)/g1^6 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 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 |