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 |
|---|---|---|---|---|---|---|---|---|---|
| 55171 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_3\phi_1^2$ + $ M_3M_4$ + $ M_5\phi_1q_2^2$ + $ M_1^2$ + $ M_6\tilde{q}_1\tilde{q}_2$ | 0.6985 | 0.8713 | 0.8016 | [X:[], M:[1.0, 0.9731, 1.1171, 0.8829, 0.7026, 0.7658], q:[0.572, 0.428], qb:[0.4549, 0.7793], phi:[0.4415]] | [X:[], M:[[0], [-18], [4], [-4], [24], [-8]], q:[[11], [-11]], qb:[[7], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_5$, $ M_6$, $ M_4$, $ \phi_1^2$, $ M_2$, $ M_1$, $ q_2\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_1\tilde{q}_2$, $ M_5^2$, $ \phi_1q_1q_2$, $ M_5M_6$, $ \phi_1q_1\tilde{q}_1$, $ M_6^2$, $ M_4M_5$, $ M_5\phi_1^2$, $ \phi_1q_1^2$, $ M_4M_6$, $ M_6\phi_1^2$, $ M_2M_5$, $ M_1M_5$, $ M_2M_6$, $ M_4^2$, $ M_1M_6$, $ M_4\phi_1^2$, $ \phi_1^4$, $ M_2M_4$, $ M_2\phi_1^2$, $ M_1M_4$, $ M_1\phi_1^2$, $ M_5q_2\tilde{q}_2$, $ M_2^2$, $ M_1M_2$, $ M_6q_2\tilde{q}_2$ | . | -2 | t^2.11 + t^2.3 + 2*t^2.65 + t^2.92 + t^3. + t^3.62 + t^3.97 + 2*t^4.05 + t^4.22 + t^4.32 + 2*t^4.41 + t^4.59 + 3*t^4.76 + 2*t^4.95 + t^5.03 + t^5.11 + t^5.22 + 4*t^5.3 + t^5.57 + t^5.65 + t^5.73 + t^5.84 + t^5.92 - 2*t^6. + 2*t^6.16 + 2*t^6.27 + t^6.32 + 2*t^6.51 + t^6.54 + 3*t^6.62 + 4*t^6.7 + 3*t^6.86 + t^6.89 + 2*t^6.97 + 5*t^7.05 + t^7.13 + t^7.22 + 2*t^7.24 + 4*t^7.41 + t^7.51 + 4*t^7.59 + t^7.68 + t^7.84 + t^7.87 + 6*t^7.95 + 2*t^8.03 - t^8.11 + t^8.14 + 2*t^8.22 + 2*t^8.27 - 2*t^8.3 + 2*t^8.38 + t^8.43 + t^8.46 + t^8.49 + t^8.57 + 2*t^8.62 - 4*t^8.65 + t^8.76 + 6*t^8.81 + t^8.84 + 2*t^8.92 + 3*t^8.97 - t^4.32/y - t^6.43/y - t^6.62/y - t^6.97/y - t^7.24/y + (2*t^7.41)/y + t^7.68/y + (2*t^7.76)/y + (2*t^7.95)/y + (2*t^8.03)/y + t^8.11/y + (2*t^8.22)/y + (2*t^8.3)/y - t^8.54/y + (2*t^8.57)/y + (2*t^8.65)/y + t^8.92/y - t^4.32*y - t^6.43*y - t^6.62*y - t^6.97*y - t^7.24*y + 2*t^7.41*y + t^7.68*y + 2*t^7.76*y + 2*t^7.95*y + 2*t^8.03*y + t^8.11*y + 2*t^8.22*y + 2*t^8.3*y - t^8.54*y + 2*t^8.57*y + 2*t^8.65*y + t^8.92*y | g1^24*t^2.11 + t^2.3/g1^8 + (2*t^2.65)/g1^4 + t^2.92/g1^18 + t^3. + t^3.62/g1^10 + t^3.97/g1^6 + 2*g1^12*t^4.05 + g1^48*t^4.22 + t^4.32/g1^2 + 2*g1^16*t^4.41 + t^4.59/g1^16 + 3*g1^20*t^4.76 + (2*t^4.95)/g1^12 + g1^6*t^5.03 + g1^24*t^5.11 + t^5.22/g1^26 + (4*t^5.3)/g1^8 + t^5.57/g1^22 + t^5.65/g1^4 + g1^14*t^5.73 + t^5.84/g1^36 + t^5.92/g1^18 - 2*t^6. + 2*g1^36*t^6.16 + (2*t^6.27)/g1^14 + g1^72*t^6.32 + 2*g1^40*t^6.51 + t^6.54/g1^28 + (3*t^6.62)/g1^10 + 4*g1^8*t^6.7 + 3*g1^44*t^6.86 + t^6.89/g1^24 + (2*t^6.97)/g1^6 + 5*g1^12*t^7.05 + g1^30*t^7.13 + g1^48*t^7.22 + (2*t^7.24)/g1^20 + 4*g1^16*t^7.41 + t^7.51/g1^34 + (4*t^7.59)/g1^16 + g1^2*t^7.68 + g1^38*t^7.84 + t^7.87/g1^30 + (6*t^7.95)/g1^12 + 2*g1^6*t^8.03 - g1^24*t^8.11 + t^8.14/g1^44 + (2*t^8.22)/g1^26 + 2*g1^60*t^8.27 - (2*t^8.3)/g1^8 + 2*g1^10*t^8.38 + g1^96*t^8.43 + g1^28*t^8.46 + t^8.49/g1^40 + t^8.57/g1^22 + 2*g1^64*t^8.62 - (4*t^8.65)/g1^4 + t^8.76/g1^54 + 6*g1^32*t^8.81 + t^8.84/g1^36 + (2*t^8.92)/g1^18 + 3*g1^68*t^8.97 - t^4.32/(g1^2*y) - (g1^22*t^6.43)/y - t^6.62/(g1^10*y) - t^6.97/(g1^6*y) - t^7.24/(g1^20*y) + (2*g1^16*t^7.41)/y + (g1^2*t^7.68)/y + (2*g1^20*t^7.76)/y + (2*t^7.95)/(g1^12*y) + (2*g1^6*t^8.03)/y + (g1^24*t^8.11)/y + (2*t^8.22)/(g1^26*y) + (2*t^8.3)/(g1^8*y) - (g1^46*t^8.54)/y + (2*t^8.57)/(g1^22*y) + (2*t^8.65)/(g1^4*y) + t^8.92/(g1^18*y) - (t^4.32*y)/g1^2 - g1^22*t^6.43*y - (t^6.62*y)/g1^10 - (t^6.97*y)/g1^6 - (t^7.24*y)/g1^20 + 2*g1^16*t^7.41*y + g1^2*t^7.68*y + 2*g1^20*t^7.76*y + (2*t^7.95*y)/g1^12 + 2*g1^6*t^8.03*y + g1^24*t^8.11*y + (2*t^8.22*y)/g1^26 + (2*t^8.3*y)/g1^8 - g1^46*t^8.54*y + (2*t^8.57*y)/g1^22 + (2*t^8.65*y)/g1^4 + (t^8.92*y)/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 |
|---|---|---|---|---|---|---|---|---|---|
| 46942 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_3\phi_1^2$ + $ M_3M_4$ + $ M_5\phi_1q_2^2$ + $ M_1^2$ | 0.6802 | 0.8389 | 0.8108 | [X:[], M:[1.0, 0.9814, 1.1152, 0.8848, 0.6914], q:[0.5669, 0.4331], qb:[0.4517, 0.7788], phi:[0.4424]] | t^2.07 + 2*t^2.65 + t^2.94 + t^3. + t^3.64 + t^3.69 + t^3.98 + 2*t^4.04 + t^4.15 + t^4.33 + t^4.38 + 3*t^4.73 + t^5.02 + t^5.07 + 3*t^5.31 + t^5.6 + t^5.65 + t^5.71 + t^5.77 + t^5.89 - 2*t^6. - t^4.33/y - t^4.33*y | detail |