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 |
|---|---|---|---|---|---|---|---|---|---|
| 60712 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ | 1.2714 | 1.4808 | 0.8586 | [X:[1.3375], M:[0.6873], q:[0.4499, 0.7627], qb:[0.5501, 0.2126], phi:[0.3375]] | [X:[[3]], M:[[15]], q:[[4], [-11]], qb:[[-4], [-7]], phi:[[3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}^{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{5}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$ | -1 | t^2.02 + t^2.06 + t^2.93 + 2*t^3. + t^3.04 + 2*t^3.94 + 3*t^4.01 + t^4.05 + t^4.09 + t^4.12 + 6*t^4.95 + 3*t^5.02 + 2*t^5.06 + t^5.1 + t^5.85 + 2*t^5.93 + 6*t^5.96 - t^6. + 5*t^6.04 + 4*t^6.07 + t^6.11 + t^6.15 + t^6.19 + 2*t^6.86 + 5*t^6.94 + 8*t^6.98 + 4*t^7.01 + 6*t^7.05 + 3*t^7.09 + 2*t^7.12 + t^7.16 + 9*t^7.88 - 3*t^7.91 + 13*t^7.95 + 8*t^7.99 + 4*t^8.02 + 4*t^8.06 + 5*t^8.1 + 4*t^8.14 + t^8.17 + t^8.21 + t^8.25 + t^8.78 + 2*t^8.85 + 14*t^8.89 - 9*t^8.93 + 22*t^8.96 - t^4.01/y - t^5.02/y - t^6.04/y - t^6.07/y - t^6.94/y - t^7.01/y - (2*t^7.05)/y + (2*t^7.99)/y - t^8.02/y + t^8.06/y - t^8.14/y + (2*t^8.93)/y + t^8.96/y - t^4.01*y - t^5.02*y - t^6.04*y - t^6.07*y - t^6.94*y - t^7.01*y - 2*t^7.05*y + 2*t^7.99*y - t^8.02*y + t^8.06*y - t^8.14*y + 2*t^8.93*y + t^8.96*y | g1^6*t^2.02 + g1^15*t^2.06 + t^2.93/g1^18 + 2*t^3. + g1^9*t^3.04 + (2*t^3.94)/g1^15 + 3*g1^3*t^4.01 + g1^12*t^4.05 + g1^21*t^4.09 + g1^30*t^4.12 + (6*t^4.95)/g1^12 + 3*g1^6*t^5.02 + 2*g1^15*t^5.06 + g1^24*t^5.1 + t^5.85/g1^36 + (2*t^5.93)/g1^18 + (6*t^5.96)/g1^9 - t^6. + 5*g1^9*t^6.04 + 4*g1^18*t^6.07 + g1^27*t^6.11 + g1^36*t^6.15 + g1^45*t^6.19 + (2*t^6.86)/g1^33 + (5*t^6.94)/g1^15 + (8*t^6.98)/g1^6 + 4*g1^3*t^7.01 + 6*g1^12*t^7.05 + 3*g1^21*t^7.09 + 2*g1^30*t^7.12 + g1^39*t^7.16 + (9*t^7.88)/g1^30 - (3*t^7.91)/g1^21 + (13*t^7.95)/g1^12 + (8*t^7.99)/g1^3 + 4*g1^6*t^8.02 + 4*g1^15*t^8.06 + 5*g1^24*t^8.1 + 4*g1^33*t^8.14 + g1^42*t^8.17 + g1^51*t^8.21 + g1^60*t^8.25 + t^8.78/g1^54 + (2*t^8.85)/g1^36 + (14*t^8.89)/g1^27 - (9*t^8.93)/g1^18 + (22*t^8.96)/g1^9 - (g1^3*t^4.01)/y - (g1^6*t^5.02)/y - (g1^9*t^6.04)/y - (g1^18*t^6.07)/y - t^6.94/(g1^15*y) - (g1^3*t^7.01)/y - (2*g1^12*t^7.05)/y + (2*t^7.99)/(g1^3*y) - (g1^6*t^8.02)/y + (g1^15*t^8.06)/y - (g1^33*t^8.14)/y + (2*t^8.93)/(g1^18*y) + t^8.96/(g1^9*y) - g1^3*t^4.01*y - g1^6*t^5.02*y - g1^9*t^6.04*y - g1^18*t^6.07*y - (t^6.94*y)/g1^15 - g1^3*t^7.01*y - 2*g1^12*t^7.05*y + (2*t^7.99*y)/g1^3 - g1^6*t^8.02*y + g1^15*t^8.06*y - g1^33*t^8.14*y + (2*t^8.93*y)/g1^18 + (t^8.96*y)/g1^9 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 57470 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ | 1.348 | 1.5616 | 0.8633 | [X:[1.354], M:[0.7701], q:[0.3455, 0.5754], qb:[0.6545, 0.3005], phi:[0.354]] | t^2.12 + t^2.31 + t^2.63 + 2*t^3. + t^3.19 + t^3.69 + 3*t^4.06 + t^4.25 + t^4.43 + t^4.62 + 3*t^4.75 + t^4.83 + t^4.86 + 3*t^5.12 + t^5.26 + 2*t^5.31 + t^5.5 + t^5.55 + 2*t^5.63 + 3*t^5.81 + 3*t^5.89 + t^5.92 - t^6. - t^4.06/y - t^5.12/y - t^4.06*y - t^5.12*y | detail |