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 |
|---|---|---|---|---|---|---|---|---|---|
| 55933 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_2^2$ + $ M_4q_1\tilde{q}_1$ + $ M_3M_5$ + $ M_2M_6$ | 0.6974 | 0.8735 | 0.7985 | [X:[], M:[0.6948, 1.1017, 0.9801, 0.7345, 1.0199, 0.8983], q:[0.7754, 0.5298], qb:[0.4901, 0.4082], phi:[0.4491]] | [X:[], M:[[36], [-12], [22], [-8], [-22], [12]], q:[[-3], [-33]], qb:[[11], [1]], phi:[[6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ M_4$, $ M_6$, $ \phi_1^2$, $ q_2\tilde{q}_2$, $ M_5$, $ q_1\tilde{q}_2$, $ q_1\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ M_1^2$, $ M_1M_4$, $ \phi_1\tilde{q}_1^2$, $ M_4^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_2^2$, $ M_1M_6$, $ M_1\phi_1^2$, $ M_4M_6$, $ M_4\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ M_4q_2\tilde{q}_2$, $ M_1M_5$, $ \phi_1q_1\tilde{q}_1$, $ M_4M_5$, $ \phi_1q_1q_2$, $ M_6^2$, $ M_6\phi_1^2$, $ \phi_1^4$, $ M_6q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_5M_6$, $ M_5\phi_1^2$, $ M_4q_1\tilde{q}_2$, $ M_5q_2\tilde{q}_2$ | . | -2 | t^2.08 + t^2.2 + 2*t^2.69 + t^2.81 + t^3.06 + t^3.55 + t^3.8 + t^4.04 + t^4.16 + t^4.17 + 2*t^4.29 + 2*t^4.41 + t^4.53 + 2*t^4.78 + 3*t^4.9 + t^5.02 + t^5.14 + t^5.26 + 3*t^5.39 + 2*t^5.51 + t^5.63 + 2*t^5.75 + t^5.87 - 2*t^6. + t^6.13 + 3*t^6.25 + t^6.36 + 2*t^6.37 + 4*t^6.49 + 3*t^6.61 + t^6.73 + t^6.74 + 4*t^6.86 + 5*t^6.98 + 4*t^7.1 + 4*t^7.22 + t^7.34 + 3*t^7.47 + 5*t^7.59 + t^7.71 + 2*t^7.84 + 3*t^7.96 + 3*t^8.08 + t^8.21 + 2*t^8.32 + t^8.33 + t^8.34 + t^8.44 + 2*t^8.45 + 2*t^8.46 + 2*t^8.57 + 3*t^8.58 + 2*t^8.82 + 2*t^8.93 + 2*t^8.94 + 2*t^8.95 - t^4.35/y - t^6.43/y - t^6.55/y - t^7.04/y + t^7.29/y + t^7.65/y + (2*t^7.78)/y + (3*t^7.9)/y + t^8.02/y + (2*t^8.14)/y + (2*t^8.26)/y + t^8.39/y + (2*t^8.51)/y - t^8.52/y + (2*t^8.75)/y + t^8.87/y + t^8.88/y - t^4.35*y - t^6.43*y - t^6.55*y - t^7.04*y + t^7.29*y + t^7.65*y + 2*t^7.78*y + 3*t^7.9*y + t^8.02*y + 2*t^8.14*y + 2*t^8.26*y + t^8.39*y + 2*t^8.51*y - t^8.52*y + 2*t^8.75*y + t^8.87*y + t^8.88*y | g1^36*t^2.08 + t^2.2/g1^8 + 2*g1^12*t^2.69 + t^2.81/g1^32 + t^3.06/g1^22 + t^3.55/g1^2 + g1^8*t^3.8 + g1^18*t^4.04 + t^4.16/g1^26 + g1^72*t^4.17 + 2*g1^28*t^4.29 + (2*t^4.41)/g1^16 + t^4.53/g1^60 + 2*g1^48*t^4.78 + 3*g1^4*t^4.9 + t^5.02/g1^40 + g1^14*t^5.14 + t^5.26/g1^30 + 3*g1^24*t^5.39 + (2*t^5.51)/g1^20 + t^5.63/g1^64 + (2*t^5.75)/g1^10 + t^5.87/g1^54 - 2*t^6. + g1^54*t^6.13 + 2*g1^10*t^6.25 + g1^108*t^6.25 + t^6.36/g1^34 + 2*g1^64*t^6.37 + 4*g1^20*t^6.49 + (3*t^6.61)/g1^24 + t^6.73/g1^68 + g1^30*t^6.74 + (2*t^6.86)/g1^14 + 2*g1^84*t^6.86 + t^6.98/g1^58 + 4*g1^40*t^6.98 + (4*t^7.1)/g1^4 + (4*t^7.22)/g1^48 + t^7.34/g1^92 + 3*g1^60*t^7.47 + t^7.59/g1^82 + 4*g1^16*t^7.59 + t^7.71/g1^28 + 2*g1^26*t^7.84 + (3*t^7.96)/g1^18 + t^8.08/g1^62 + 2*g1^36*t^8.08 + g1^90*t^8.21 + (2*t^8.32)/g1^52 + g1^46*t^8.33 + g1^144*t^8.34 + t^8.44/g1^96 + 2*g1^2*t^8.45 + 2*g1^100*t^8.46 + (2*t^8.57)/g1^42 + 3*g1^56*t^8.58 + (2*t^8.69)/g1^86 - 2*g1^12*t^8.69 + 2*g1^66*t^8.82 + (2*t^8.93)/g1^76 + 2*g1^22*t^8.94 + 2*g1^120*t^8.95 - (g1^6*t^4.35)/y - (g1^42*t^6.43)/y - t^6.55/(g1^2*y) - (g1^18*t^7.04)/y + (g1^28*t^7.29)/y + t^7.65/(g1^6*y) + (2*g1^48*t^7.78)/y + (3*g1^4*t^7.9)/y + t^8.02/(g1^40*y) + (2*g1^14*t^8.14)/y + (2*t^8.26)/(g1^30*y) + (g1^24*t^8.39)/y + (2*t^8.51)/(g1^20*y) - (g1^78*t^8.52)/y + (2*t^8.75)/(g1^10*y) + t^8.87/(g1^54*y) + (g1^44*t^8.88)/y - g1^6*t^4.35*y - g1^42*t^6.43*y - (t^6.55*y)/g1^2 - g1^18*t^7.04*y + g1^28*t^7.29*y + (t^7.65*y)/g1^6 + 2*g1^48*t^7.78*y + 3*g1^4*t^7.9*y + (t^8.02*y)/g1^40 + 2*g1^14*t^8.14*y + (2*t^8.26*y)/g1^30 + g1^24*t^8.39*y + (2*t^8.51*y)/g1^20 - g1^78*t^8.52*y + (2*t^8.75*y)/g1^10 + (t^8.87*y)/g1^54 + g1^44*t^8.88*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 |
|---|---|---|---|---|---|---|---|---|---|
| 48188 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_2^2$ + $ M_4q_1\tilde{q}_1$ + $ M_3M_5$ | 0.6884 | 0.8584 | 0.802 | [X:[], M:[0.7083, 1.0972, 0.9884, 0.7315, 1.0116], q:[0.7743, 0.5174], qb:[0.4942, 0.4086], phi:[0.4514]] | t^2.12 + t^2.19 + t^2.71 + t^2.78 + t^3.03 + t^3.29 + t^3.55 + t^3.81 + t^4.06 + t^4.13 + t^4.25 + 2*t^4.32 + 2*t^4.39 + t^4.46 + t^4.83 + 2*t^4.9 + t^4.97 + t^5.16 + t^5.23 + 2*t^5.42 + 2*t^5.49 + t^5.56 + t^5.74 + t^5.81 - t^6. - t^4.35/y - t^4.35*y | detail |