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 |
|---|---|---|---|---|---|---|---|---|---|
| 55292 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.593 | 0.7591 | 0.7812 | [X:[], M:[0.6851, 1.105, 0.79, 1.105, 1.105, 0.79], q:[0.7762, 0.5387], qb:[0.6713, 0.2238], phi:[0.4475]] | [X:[], M:[[12], [-4], [8], [-4], [-4], [8]], q:[[-1], [-11]], qb:[[3], [1]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{6}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$ | ${}$ | -4 | t^2.06 + t^2.29 + 2*t^2.37 + t^3. + 3*t^3.31 + t^4.03 + t^4.11 + 2*t^4.34 + 2*t^4.43 + 2*t^4.57 + t^4.66 + 3*t^4.74 + t^4.97 + t^5.29 + 6*t^5.37 + 2*t^5.6 + 5*t^5.69 - 4*t^6. + t^6.08 + t^6.17 + 2*t^6.31 + 2*t^6.4 + 2*t^6.48 + 6*t^6.63 + 2*t^6.71 + 3*t^6.8 + 2*t^6.86 + t^7.03 + 4*t^7.11 - t^7.26 + 2*t^7.34 + 4*t^7.43 + t^7.57 + 3*t^7.66 + 9*t^7.74 + 4*t^7.89 + 2*t^8.06 + t^8.14 + t^8.22 - 2*t^8.29 - 7*t^8.37 + 2*t^8.45 + 2*t^8.54 + t^8.6 + 10*t^8.69 + 2*t^8.77 + 3*t^8.85 + 3*t^8.92 - t^4.34/y - t^6.4/y - (2*t^6.71)/y + (2*t^7.03)/y + t^7.34/y + (2*t^7.43)/y + t^7.74/y + (2*t^7.97)/y + t^8.06/y + (2*t^8.29)/y + (5*t^8.37)/y - t^8.45/y + (3*t^8.6)/y + (6*t^8.69)/y - (2*t^8.77)/y - t^4.34*y - t^6.4*y - 2*t^6.71*y + 2*t^7.03*y + t^7.34*y + 2*t^7.43*y + t^7.74*y + 2*t^7.97*y + t^8.06*y + 2*t^8.29*y + 5*t^8.37*y - t^8.45*y + 3*t^8.6*y + 6*t^8.69*y - 2*t^8.77*y | g1^12*t^2.06 + t^2.29/g1^10 + 2*g1^8*t^2.37 + t^3. + (3*t^3.31)/g1^4 + g1^6*t^4.03 + g1^24*t^4.11 + 2*g1^2*t^4.34 + 2*g1^20*t^4.43 + (2*t^4.57)/g1^20 + t^4.66/g1^2 + 3*g1^16*t^4.74 + t^4.97/g1^6 + t^5.29/g1^10 + 6*g1^8*t^5.37 + (2*t^5.6)/g1^14 + 5*g1^4*t^5.69 - 4*t^6. + g1^18*t^6.08 + g1^36*t^6.17 + (2*t^6.31)/g1^4 + 2*g1^14*t^6.4 + 2*g1^32*t^6.48 + (6*t^6.63)/g1^8 + 2*g1^10*t^6.71 + 3*g1^28*t^6.8 + (2*t^6.86)/g1^30 + g1^6*t^7.03 + 4*g1^24*t^7.11 - t^7.26/g1^16 + 2*g1^2*t^7.34 + 4*g1^20*t^7.43 + t^7.57/g1^20 + (3*t^7.66)/g1^2 + 9*g1^16*t^7.74 + (4*t^7.89)/g1^24 + 2*g1^12*t^8.06 + g1^30*t^8.14 + g1^48*t^8.22 - (2*t^8.29)/g1^10 - 7*g1^8*t^8.37 + 2*g1^26*t^8.45 + 2*g1^44*t^8.54 + t^8.6/g1^14 + 10*g1^4*t^8.69 + 2*g1^22*t^8.77 + 3*g1^40*t^8.85 + (3*t^8.92)/g1^18 - (g1^2*t^4.34)/y - (g1^14*t^6.4)/y - (2*g1^10*t^6.71)/y + (2*g1^6*t^7.03)/y + (g1^2*t^7.34)/y + (2*g1^20*t^7.43)/y + (g1^16*t^7.74)/y + (2*t^7.97)/(g1^6*y) + (g1^12*t^8.06)/y + (2*t^8.29)/(g1^10*y) + (5*g1^8*t^8.37)/y - (g1^26*t^8.45)/y + (3*t^8.6)/(g1^14*y) + (6*g1^4*t^8.69)/y - (2*g1^22*t^8.77)/y - g1^2*t^4.34*y - g1^14*t^6.4*y - 2*g1^10*t^6.71*y + 2*g1^6*t^7.03*y + g1^2*t^7.34*y + 2*g1^20*t^7.43*y + g1^16*t^7.74*y + (2*t^7.97*y)/g1^6 + g1^12*t^8.06*y + (2*t^8.29*y)/g1^10 + 5*g1^8*t^8.37*y - g1^26*t^8.45*y + (3*t^8.6*y)/g1^14 + 6*g1^4*t^8.69*y - 2*g1^22*t^8.77*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46928 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}\phi_{1}^{2}$ | 0.5762 | 0.7294 | 0.79 | [X:[], M:[0.7029, 1.099, 0.8019, 1.099, 1.099], q:[0.7748, 0.5223], qb:[0.6757, 0.2252], phi:[0.4505]] | t^2.11 + t^2.24 + t^2.41 + t^3. + 3*t^3.3 + t^3.59 + t^4.05 + t^4.22 + 2*t^4.35 + 2*t^4.49 + t^4.51 + t^4.81 + t^4.95 + t^5.24 + 5*t^5.41 + 2*t^5.54 + 3*t^5.7 + t^5.84 - 3*t^6. - t^4.35/y - t^4.35*y | detail |