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 |
|---|---|---|---|---|---|---|---|---|---|
| 57946 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ | 1.4311 | 1.6153 | 0.886 | [X:[1.3797], M:[0.7753], q:[0.4441, 0.615], qb:[0.4705, 0.6097], phi:[0.3101]] | [X:[[12]], M:[[-15]], q:[[43], [1]], qb:[[-22], [14]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | ${}$ | -1 | t^2.33 + t^2.74 + t^2.79 + t^3.16 + t^3.26 + t^3.67 + t^4.09 + t^4.14 + t^4.19 + 2*t^4.6 + t^4.65 + t^5.02 + t^5.07 + 2*t^5.12 + t^5.44 + t^5.49 + 2*t^5.53 + 2*t^5.58 + t^5.9 + 2*t^5.95 - t^6. + t^6.05 + t^6.32 + t^6.37 + t^6.42 + 2*t^6.47 + t^6.51 + t^6.79 + 2*t^6.84 + 3*t^6.88 + 3*t^6.93 + 2*t^6.98 + t^7.03 + t^7.25 + 2*t^7.3 + 3*t^7.35 + 3*t^7.4 + 2*t^7.44 + 3*t^7.77 + 3*t^7.81 + 5*t^7.86 + t^7.91 + 2*t^8.18 + 2*t^8.23 + 6*t^8.28 + t^8.33 + 3*t^8.37 - t^8.42 + t^8.6 + t^8.65 + 5*t^8.7 + 4*t^8.79 + t^8.79/y^2 - t^3.93/y - t^4.86/y - t^6.26/y - t^6.67/y - t^6.72/y - t^7.09/y - (2*t^7.19)/y - t^7.6/y - t^7.65/y - t^8.02/y + t^8.07/y + t^8.49/y + t^8.9/y - t^3.93*y - t^4.86*y - t^6.26*y - t^6.67*y - t^6.72*y - t^7.09*y - 2*t^7.19*y - t^7.6*y - t^7.65*y - t^8.02*y + t^8.07*y + t^8.49*y + t^8.9*y + t^8.79*y^2 | t^2.33/g1^15 + g1^21*t^2.74 + t^2.79/g1^18 + g1^57*t^3.16 + t^3.26/g1^21 + g1^15*t^3.67 + g1^51*t^4.09 + g1^12*t^4.14 + t^4.19/g1^27 + 2*g1^9*t^4.6 + t^4.65/g1^30 + g1^45*t^5.02 + g1^6*t^5.07 + (2*t^5.12)/g1^33 + g1^81*t^5.44 + g1^42*t^5.49 + 2*g1^3*t^5.53 + (2*t^5.58)/g1^36 + g1^78*t^5.9 + 2*g1^39*t^5.95 - t^6. + t^6.05/g1^39 + g1^114*t^6.32 + g1^75*t^6.37 + g1^36*t^6.42 + (2*t^6.47)/g1^3 + t^6.51/g1^42 + g1^111*t^6.79 + 2*g1^72*t^6.84 + 3*g1^33*t^6.88 + (3*t^6.93)/g1^6 + (2*t^6.98)/g1^45 + t^7.03/g1^84 + g1^108*t^7.25 + 2*g1^69*t^7.3 + 3*g1^30*t^7.35 + (3*t^7.4)/g1^9 + (2*t^7.44)/g1^48 + 3*g1^66*t^7.77 + 3*g1^27*t^7.81 + (5*t^7.86)/g1^12 + t^7.91/g1^51 + 2*g1^102*t^8.18 + 2*g1^63*t^8.23 + 6*g1^24*t^8.28 + t^8.33/g1^15 + (3*t^8.37)/g1^54 - t^8.42/g1^93 + g1^138*t^8.6 + g1^99*t^8.65 + 5*g1^60*t^8.7 + (4*t^8.79)/g1^18 + t^8.79/(g1^18*y^2) - t^3.93/(g1^6*y) - t^4.86/(g1^12*y) - t^6.26/(g1^21*y) - (g1^15*t^6.67)/y - t^6.72/(g1^24*y) - (g1^51*t^7.09)/y - (2*t^7.19)/(g1^27*y) - (g1^9*t^7.6)/y - t^7.65/(g1^30*y) - (g1^45*t^8.02)/y + (g1^6*t^8.07)/y + (g1^42*t^8.49)/y + (g1^78*t^8.9)/y - (t^3.93*y)/g1^6 - (t^4.86*y)/g1^12 - (t^6.26*y)/g1^21 - g1^15*t^6.67*y - (t^6.72*y)/g1^24 - g1^51*t^7.09*y - (2*t^7.19*y)/g1^27 - g1^9*t^7.6*y - (t^7.65*y)/g1^30 - g1^45*t^8.02*y + g1^6*t^8.07*y + g1^42*t^8.49*y + g1^78*t^8.9*y + (t^8.79*y^2)/g1^18 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 57302 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1.4334 | 1.623 | 0.8832 | [X:[1.3613], M:[0.7984], q:[0.4354, 0.5847], qb:[0.4469, 0.6169], phi:[0.3194]] | t^2.395 + t^2.647 + t^2.874 + t^3.095 + t^3.157 + t^3.605 + t^4.053 + t^4.084 + t^4.115 + 2*t^4.563 + t^4.79 + t^5.011 + t^5.042 + t^5.073 + t^5.269 + t^5.293 + t^5.324 + t^5.49 + 2*t^5.521 + t^5.741 + t^5.748 + t^5.773 + t^5.804 + t^5.969 - 2*t^6. - t^3.958/y - t^4.916/y - t^3.958*y - t^4.916*y | detail |