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 |
|---|---|---|---|---|---|---|---|---|---|
| 59423 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.4387 | 1.63 | 0.8826 | [X:[1.3251], M:[0.9876], q:[0.4334, 0.4458], qb:[0.5666, 0.5294], phi:[0.3375]] | [X:[[6]], M:[[9]], q:[[8], [-1]], qb:[[-8], [19]], phi:[[-3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${}\phi_{1}^{2}q_{1}q_{2}^{2}$ | 0 | t^2.89 + t^2.93 + t^2.96 + t^3. + t^3.04 + t^3.9 + t^3.94 + t^3.98 + t^4.01 + t^4.05 + t^4.91 + 2*t^4.95 + t^4.99 + t^5.02 + t^5.06 + t^5.78 + t^5.81 + 2*t^5.85 + 2*t^5.89 + 3*t^5.93 + 2*t^5.96 + t^6.07 - t^6.11 + t^6.79 + 2*t^6.83 + 3*t^6.86 + 4*t^6.9 + 5*t^6.94 + 4*t^6.98 + 2*t^7.01 + t^7.05 + t^7.09 - t^7.12 + 3*t^7.8 + 4*t^7.84 + 5*t^7.88 + 5*t^7.91 + 5*t^7.95 + 3*t^7.99 + 2*t^8.02 + t^8.1 + t^8.67 + t^8.7 + 2*t^8.74 + 3*t^8.78 + 5*t^8.81 + 6*t^8.85 + 4*t^8.89 + 3*t^8.93 + 2*t^8.96 - t^4.01/y - t^5.02/y - t^6.9/y - t^6.94/y - t^6.98/y - t^7.01/y - t^7.05/y - t^7.91/y - t^7.95/y - t^7.99/y - t^8.02/y - t^8.06/y + t^8.81/y + t^8.85/y + (2*t^8.89)/y + t^8.93/y + t^8.96/y - t^4.01*y - t^5.02*y - t^6.9*y - t^6.94*y - t^6.98*y - t^7.01*y - t^7.05*y - t^7.91*y - t^7.95*y - t^7.99*y - t^8.02*y - t^8.06*y + t^8.81*y + t^8.85*y + 2*t^8.89*y + t^8.93*y + t^8.96*y | g1^27*t^2.89 + g1^18*t^2.93 + g1^9*t^2.96 + t^3. + t^3.04/g1^9 + g1^24*t^3.9 + g1^15*t^3.94 + g1^6*t^3.98 + t^4.01/g1^3 + t^4.05/g1^12 + g1^21*t^4.91 + 2*g1^12*t^4.95 + g1^3*t^4.99 + t^5.02/g1^6 + t^5.06/g1^15 + g1^54*t^5.78 + g1^45*t^5.81 + 2*g1^36*t^5.85 + 2*g1^27*t^5.89 + 3*g1^18*t^5.93 + 2*g1^9*t^5.96 + t^6.07/g1^18 - t^6.11/g1^27 + g1^51*t^6.79 + 2*g1^42*t^6.83 + 3*g1^33*t^6.86 + 4*g1^24*t^6.9 + 5*g1^15*t^6.94 + 4*g1^6*t^6.98 + (2*t^7.01)/g1^3 + t^7.05/g1^12 + t^7.09/g1^21 - t^7.12/g1^30 + 3*g1^48*t^7.8 + 4*g1^39*t^7.84 + 5*g1^30*t^7.88 + 5*g1^21*t^7.91 + 5*g1^12*t^7.95 + 3*g1^3*t^7.99 + (2*t^8.02)/g1^6 + t^8.1/g1^24 + g1^81*t^8.67 + g1^72*t^8.7 + 2*g1^63*t^8.74 + 3*g1^54*t^8.78 + 5*g1^45*t^8.81 + 6*g1^36*t^8.85 + 4*g1^27*t^8.89 + 3*g1^18*t^8.93 + 2*g1^9*t^8.96 - t^4.01/(g1^3*y) - t^5.02/(g1^6*y) - (g1^24*t^6.9)/y - (g1^15*t^6.94)/y - (g1^6*t^6.98)/y - t^7.01/(g1^3*y) - t^7.05/(g1^12*y) - (g1^21*t^7.91)/y - (g1^12*t^7.95)/y - (g1^3*t^7.99)/y - t^8.02/(g1^6*y) - t^8.06/(g1^15*y) + (g1^45*t^8.81)/y + (g1^36*t^8.85)/y + (2*g1^27*t^8.89)/y + (g1^18*t^8.93)/y + (g1^9*t^8.96)/y - (t^4.01*y)/g1^3 - (t^5.02*y)/g1^6 - g1^24*t^6.9*y - g1^15*t^6.94*y - g1^6*t^6.98*y - (t^7.01*y)/g1^3 - (t^7.05*y)/g1^12 - g1^21*t^7.91*y - g1^12*t^7.95*y - g1^3*t^7.99*y - (t^8.02*y)/g1^6 - (t^8.06*y)/g1^15 + g1^45*t^8.81*y + g1^36*t^8.85*y + 2*g1^27*t^8.89*y + g1^18*t^8.93*y + g1^9*t^8.96*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57613 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.4453 | 1.6323 | 0.8855 | [X:[1.3487], M:[0.916], q:[0.4293, 0.5133], qb:[0.5707, 0.5329], phi:[0.3256]] | t^2.75 + t^2.89 + t^2.93 + t^3. + t^3.14 + t^3.86 + t^3.98 + t^4.05 + t^4.12 + t^4.23 + t^4.84 + t^4.95 + 2*t^5.09 + t^5.21 + t^5.34 + t^5.5 + t^5.63 + t^5.68 + t^5.77 + t^5.82 + t^5.86 + 2*t^5.89 + t^5.93 - 2*t^6. - t^3.98/y - t^4.95/y - t^3.98*y - t^4.95*y | detail |