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 |
|---|---|---|---|---|---|---|---|---|---|
| 4216 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_4\phi_1q_2^2$ + $ M_4q_1\tilde{q}_2$ + $ M_1M_5$ + $ M_4M_6$ + $ M_7q_1\tilde{q}_1$ + $ M_8q_1q_2$ | 0.6863 | 0.8527 | 0.8049 | [X:[], M:[1.045, 1.1081, 0.9684, 0.7388, 0.955, 1.2612, 0.6756, 0.8153], q:[0.777, 0.4077], qb:[0.5474, 0.4842], phi:[0.4459]] | [X:[], M:[[32], [-12], [22], [-8], [-32], [8], [36], [2]], q:[[-3], [1]], qb:[[-33], [11]], phi:[[6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_7$, $ M_8$, $ \phi_1^2$, $ M_5$, $ M_3$, $ M_2$, $ M_6$, $ q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ M_7^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_7M_8$, $ \phi_1\tilde{q}_1^2$, $ M_7\phi_1^2$, $ M_5M_7$, $ M_8^2$, $ M_3M_7$, $ M_8\phi_1^2$, $ M_5M_8$, $ M_2M_7$, $ M_3M_8$, $ \phi_1^4$, $ M_5\phi_1^2$, $ M_5^2$, $ M_3M_5$, $ M_2M_8$, $ M_3^2$, $ M_6M_7$, $ M_7q_1\tilde{q}_2$ | . | -2 | t^2.03 + t^2.45 + t^2.68 + t^2.87 + t^2.91 + t^3.32 + 2*t^3.78 + t^4.01 + t^4.05 + t^4.2 + t^4.24 + t^4.43 + t^4.47 + t^4.62 + t^4.7 + 2*t^4.89 + t^4.93 + t^5.12 + t^5.31 + 3*t^5.35 + t^5.54 + t^5.73 + t^5.77 + 2*t^5.81 - 2*t^6. + t^6.04 + t^6.08 + 2*t^6.23 + t^6.27 - t^6.42 + 3*t^6.46 + t^6.5 + 3*t^6.65 + 3*t^6.69 + t^6.73 + t^6.88 + 3*t^6.92 + t^6.96 + 2*t^7.07 + t^7.11 + t^7.15 + t^7.3 + t^7.34 + 3*t^7.38 + t^7.49 + 3*t^7.57 + 4*t^7.8 + 2*t^7.84 + t^7.99 + t^8.03 + t^8.07 + t^8.11 + 2*t^8.22 + 3*t^8.26 + t^8.3 + 2*t^8.41 - 4*t^8.45 + 3*t^8.49 + t^8.53 + t^8.6 + 2*t^8.68 + 4*t^8.72 + t^8.76 + t^8.82 - 3*t^8.87 - t^8.91 + 3*t^8.95 + t^8.99 - t^4.34/y - t^6.36/y - t^6.78/y - t^7.24/y + t^7.43/y + t^7.47/y + t^7.7/y + (2*t^7.89)/y + t^7.93/y + t^8.12/y + (2*t^8.31)/y + (2*t^8.35)/y - t^8.39/y + t^8.54/y + t^8.58/y + (2*t^8.77)/y + t^8.81/y - t^4.34*y - t^6.36*y - t^6.78*y - t^7.24*y + t^7.43*y + t^7.47*y + t^7.7*y + 2*t^7.89*y + t^7.93*y + t^8.12*y + 2*t^8.31*y + 2*t^8.35*y - t^8.39*y + t^8.54*y + t^8.58*y + 2*t^8.77*y + t^8.81*y | g1^36*t^2.03 + g1^2*t^2.45 + g1^12*t^2.68 + t^2.87/g1^32 + g1^22*t^2.91 + t^3.32/g1^12 + 2*g1^8*t^3.78 + g1^18*t^4.01 + g1^72*t^4.05 + t^4.2/g1^26 + g1^28*t^4.24 + t^4.43/g1^16 + g1^38*t^4.47 + t^4.62/g1^60 + g1^48*t^4.7 + 2*g1^4*t^4.89 + g1^58*t^4.93 + g1^14*t^5.12 + t^5.31/g1^30 + 3*g1^24*t^5.35 + t^5.54/g1^20 + t^5.73/g1^64 + t^5.77/g1^10 + 2*g1^44*t^5.81 - 2*t^6. + g1^54*t^6.04 + g1^108*t^6.08 + 2*g1^10*t^6.23 + g1^64*t^6.27 - t^6.42/g1^34 + 3*g1^20*t^6.46 + g1^74*t^6.5 + (3*t^6.65)/g1^24 + 3*g1^30*t^6.69 + g1^84*t^6.73 + t^6.88/g1^14 + 3*g1^40*t^6.92 + g1^94*t^6.96 + (2*t^7.07)/g1^58 + t^7.11/g1^4 + g1^50*t^7.15 + t^7.3/g1^48 + g1^6*t^7.34 + 3*g1^60*t^7.38 + t^7.49/g1^92 + 3*g1^16*t^7.57 + 4*g1^26*t^7.8 + 2*g1^80*t^7.84 + t^7.99/g1^18 + g1^36*t^8.03 + g1^90*t^8.07 + g1^144*t^8.11 + (2*t^8.22)/g1^8 + 3*g1^46*t^8.26 + g1^100*t^8.3 + (2*t^8.41)/g1^52 - 4*g1^2*t^8.45 + 3*g1^56*t^8.49 + g1^110*t^8.53 + t^8.6/g1^96 + 2*g1^12*t^8.68 + 4*g1^66*t^8.72 + g1^120*t^8.76 + t^8.82/g1^86 - (3*t^8.87)/g1^32 - g1^22*t^8.91 + 3*g1^76*t^8.95 + g1^130*t^8.99 - (g1^6*t^4.34)/y - (g1^42*t^6.36)/y - (g1^8*t^6.78)/y - (g1^28*t^7.24)/y + t^7.43/(g1^16*y) + (g1^38*t^7.47)/y + (g1^48*t^7.7)/y + (2*g1^4*t^7.89)/y + (g1^58*t^7.93)/y + (g1^14*t^8.12)/y + (2*t^8.31)/(g1^30*y) + (2*g1^24*t^8.35)/y - (g1^78*t^8.39)/y + t^8.54/(g1^20*y) + (g1^34*t^8.58)/y + (2*t^8.77)/(g1^10*y) + (g1^44*t^8.81)/y - g1^6*t^4.34*y - g1^42*t^6.36*y - g1^8*t^6.78*y - g1^28*t^7.24*y + (t^7.43*y)/g1^16 + g1^38*t^7.47*y + g1^48*t^7.7*y + 2*g1^4*t^7.89*y + g1^58*t^7.93*y + g1^14*t^8.12*y + (2*t^8.31*y)/g1^30 + 2*g1^24*t^8.35*y - g1^78*t^8.39*y + (t^8.54*y)/g1^20 + g1^34*t^8.58*y + (2*t^8.77*y)/g1^10 + g1^44*t^8.81*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2214 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_4\phi_1q_2^2$ + $ M_4q_1\tilde{q}_2$ + $ M_1M_5$ + $ M_4M_6$ + $ M_7q_1\tilde{q}_1$ | 0.6708 | 0.8256 | 0.8125 | [X:[], M:[1.0465, 1.1076, 0.9695, 0.7384, 0.9535, 1.2616, 0.6773], q:[0.7769, 0.4077], qb:[0.5458, 0.4847], phi:[0.4462]] | t^2.03 + t^2.68 + t^2.86 + t^2.91 + t^3.32 + t^3.55 + 2*t^3.78 + t^4.02 + t^4.06 + t^4.2 + t^4.25 + t^4.43 + t^4.61 + t^4.71 + t^4.89 + t^4.94 + 2*t^5.35 + t^5.54 + t^5.59 + t^5.72 + 2*t^5.82 - 2*t^6. - t^4.34/y - t^4.34*y | detail |