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 |
|---|---|---|---|---|---|---|---|---|---|
| 58375 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1.3396 | 1.5776 | 0.8491 | [X:[1.4], M:[0.7922], q:[0.2693, 0.4615], qb:[0.5385, 0.3307], 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 |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$ | 2 | 2*t^2.38 + t^2.4 + t^2.42 + 2*t^3. + t^3.58 + t^3.6 + 4*t^4.2 + 3*t^4.75 + 4*t^4.78 + 4*t^4.8 + 2*t^4.82 + t^4.85 + 3*t^5.38 + 4*t^5.4 + 2*t^5.42 + 2*t^5.95 + 4*t^5.98 + 2*t^6. + 2*t^6.02 + 8*t^6.58 + 6*t^6.6 + 3*t^6.62 + 4*t^7.13 + 8*t^7.15 + 10*t^7.18 + 12*t^7.2 + 3*t^7.22 + 2*t^7.25 + t^7.27 + 5*t^7.75 + 10*t^7.78 + 8*t^7.8 + 4*t^7.82 + 2*t^7.85 + 3*t^8.33 + 8*t^8.35 + 4*t^8.38 + 14*t^8.4 - t^8.42 + 3*t^8.45 + 11*t^8.95 + 16*t^8.98 - t^4.2/y - t^5.4/y - (2*t^6.58)/y - t^6.6/y - t^6.62/y - t^7.2/y + t^7.75/y + t^7.8/y + t^7.82/y + (4*t^8.38)/y - t^8.4/y + (2*t^8.42)/y - t^8.95/y - t^4.2*y - t^5.4*y - 2*t^6.58*y - t^6.6*y - t^6.62*y - t^7.2*y + t^7.75*y + t^7.8*y + t^7.82*y + 4*t^8.38*y - t^8.4*y + 2*t^8.42*y - t^8.95*y | 2*g1^3*t^2.38 + t^2.4 + t^2.42/g1^3 + 2*t^3. + g1^3*t^3.58 + t^3.6 + 4*t^4.2 + 3*g1^6*t^4.75 + 4*g1^3*t^4.78 + 4*t^4.8 + (2*t^4.82)/g1^3 + t^4.85/g1^6 + 3*g1^3*t^5.38 + 4*t^5.4 + (2*t^5.42)/g1^3 + 2*g1^6*t^5.95 + 4*g1^3*t^5.98 + 2*t^6. + (2*t^6.02)/g1^3 + 8*g1^3*t^6.58 + 6*t^6.6 + (3*t^6.62)/g1^3 + 4*g1^9*t^7.13 + 8*g1^6*t^7.15 + 10*g1^3*t^7.18 + 12*t^7.2 + (3*t^7.22)/g1^3 + (2*t^7.25)/g1^6 + t^7.27/g1^9 + 5*g1^6*t^7.75 + 10*g1^3*t^7.78 + 8*t^7.8 + (4*t^7.82)/g1^3 + (2*t^7.85)/g1^6 + 3*g1^9*t^8.33 + 8*g1^6*t^8.35 + 4*g1^3*t^8.38 + 14*t^8.4 - t^8.42/g1^3 + (3*t^8.45)/g1^6 + 11*g1^6*t^8.95 + 16*g1^3*t^8.98 - t^4.2/y - t^5.4/y - (2*g1^3*t^6.58)/y - t^6.6/y - t^6.62/(g1^3*y) - t^7.2/y + (g1^6*t^7.75)/y + t^7.8/y + t^7.82/(g1^3*y) + (4*g1^3*t^8.38)/y - t^8.4/y + (2*t^8.42)/(g1^3*y) - (g1^6*t^8.95)/y - t^4.2*y - t^5.4*y - 2*g1^3*t^6.58*y - t^6.6*y - (t^6.62*y)/g1^3 - t^7.2*y + g1^6*t^7.75*y + t^7.8*y + (t^7.82*y)/g1^3 + 4*g1^3*t^8.38*y - t^8.4*y + (2*t^8.42*y)/g1^3 - g1^6*t^8.95*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 |