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 |
|---|---|---|---|---|---|---|---|---|---|
| 58490 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ | 1.4396 | 1.6298 | 0.8833 | [X:[1.3275], M:[0.9913], q:[0.5198, 0.572], qb:[0.4541, 0.4367], phi:[0.3362]] | [X:[[6]], M:[[9]], q:[[37], [-17]], qb:[[-10], [8]], phi:[[-3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$ | ${}\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 0 | t^2.87 + t^2.92 + t^2.97 + t^3.03 + t^3.08 + t^3.88 + t^3.93 + t^3.98 + t^4.03 + t^4.09 + t^4.89 + t^4.94 + t^4.99 + 2*t^5.04 + t^5.1 + t^5.74 + t^5.79 + 2*t^5.84 + 2*t^5.9 + 2*t^5.95 + 2*t^6.05 + t^6.1 + t^6.75 + 2*t^6.8 + 3*t^6.85 + 4*t^6.9 + 4*t^6.96 + 3*t^7.01 + 3*t^7.06 + 2*t^7.11 + t^7.7 + 2*t^7.76 + 3*t^7.81 + 4*t^7.86 + 4*t^7.91 + 4*t^7.97 + 4*t^8.02 + 3*t^8.07 + 2*t^8.12 + t^8.17 + t^8.61 + t^8.66 + 2*t^8.71 + 3*t^8.77 + 4*t^8.82 + 3*t^8.87 + 3*t^8.92 + 2*t^8.97 - t^4.01/y - t^5.02/y - t^6.88/y - t^6.93/y - t^6.98/y - t^7.03/y - t^7.09/y - t^7.89/y - t^7.94/y - t^7.99/y - t^8.04/y - t^8.1/y + t^8.79/y + t^8.84/y + t^8.9/y + t^8.95/y - t^4.01*y - t^5.02*y - t^6.88*y - t^6.93*y - t^6.98*y - t^7.03*y - t^7.09*y - t^7.89*y - t^7.94*y - t^7.99*y - t^8.04*y - t^8.1*y + t^8.79*y + t^8.84*y + t^8.9*y + t^8.95*y | g1^45*t^2.87 + g1^27*t^2.92 + g1^9*t^2.97 + t^3.03/g1^9 + t^3.08/g1^27 + g1^42*t^3.88 + g1^24*t^3.93 + g1^6*t^3.98 + t^4.03/g1^12 + t^4.09/g1^30 + g1^39*t^4.89 + g1^21*t^4.94 + g1^3*t^4.99 + (2*t^5.04)/g1^15 + t^5.1/g1^33 + g1^90*t^5.74 + g1^72*t^5.79 + 2*g1^54*t^5.84 + 2*g1^36*t^5.9 + 2*g1^18*t^5.95 + (2*t^6.05)/g1^18 + t^6.1/g1^36 + g1^87*t^6.75 + 2*g1^69*t^6.8 + 3*g1^51*t^6.85 + 4*g1^33*t^6.9 + 4*g1^15*t^6.96 + (3*t^7.01)/g1^3 + (3*t^7.06)/g1^21 + (2*t^7.11)/g1^39 + g1^102*t^7.7 + 2*g1^84*t^7.76 + 3*g1^66*t^7.81 + 4*g1^48*t^7.86 + 4*g1^30*t^7.91 + 4*g1^12*t^7.97 + (4*t^8.02)/g1^6 + (3*t^8.07)/g1^24 + (2*t^8.12)/g1^42 + t^8.17/g1^60 + g1^135*t^8.61 + g1^117*t^8.66 + 2*g1^99*t^8.71 + 3*g1^81*t^8.77 + 4*g1^63*t^8.82 + 3*g1^45*t^8.87 + 3*g1^27*t^8.92 + 2*g1^9*t^8.97 - t^4.01/(g1^3*y) - t^5.02/(g1^6*y) - (g1^42*t^6.88)/y - (g1^24*t^6.93)/y - (g1^6*t^6.98)/y - t^7.03/(g1^12*y) - t^7.09/(g1^30*y) - (g1^39*t^7.89)/y - (g1^21*t^7.94)/y - (g1^3*t^7.99)/y - t^8.04/(g1^15*y) - t^8.1/(g1^33*y) + (g1^72*t^8.79)/y + (g1^54*t^8.84)/y + (g1^36*t^8.9)/y + (g1^18*t^8.95)/y - (t^4.01*y)/g1^3 - (t^5.02*y)/g1^6 - g1^42*t^6.88*y - g1^24*t^6.93*y - g1^6*t^6.98*y - (t^7.03*y)/g1^12 - (t^7.09*y)/g1^30 - g1^39*t^7.89*y - g1^21*t^7.94*y - g1^3*t^7.99*y - (t^8.04*y)/g1^15 - (t^8.1*y)/g1^33 + g1^72*t^8.79*y + g1^54*t^8.84*y + g1^36*t^8.9*y + g1^18*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57384 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.4533 | 1.6416 | 0.8853 | [X:[1.3316], M:[0.9974], q:[0.4909, 0.5065], qb:[0.5013, 0.4961], phi:[0.3342]] | t^2.961 + t^2.977 + t^2.992 + t^3.008 + t^3.023 + t^3.964 + t^3.979 + t^3.995 + t^4.01 + t^4.026 + t^4.966 + t^4.982 + t^5.013 + t^5.029 + t^5.468 + t^5.483 + t^5.498 + t^5.515 + t^5.922 + t^5.938 + t^5.953 + 2*t^5.969 + 2*t^5.984 - 2*t^6. - t^4.003/y - t^5.005/y - t^4.003*y - t^5.005*y | detail |