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 |
|---|---|---|---|---|---|---|---|---|---|
| 3885 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1q_1\tilde{q}_2$ + $ M_6\phi_1\tilde{q}_1^2$ + $ M_3X_1$ + $ M_5M_7$ + $ M_6^2$ | 0.618 | 0.7842 | 0.7881 | [X:[1.097], M:[0.7324, 0.9264, 0.903, 0.7559, 1.2441, 1.0, 0.7559], q:[0.8044, 0.4632], qb:[0.2926, 0.7809], phi:[0.4147]] | [X:[[14]], M:[[-18], [10], [-14], [6], [-6], [0], [6]], q:[[13], [5]], qb:[[1], [-11]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ M_4$, $ M_7$, $ \phi_1^2$, $ M_2$, $ M_6$, $ X_1$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_2^2$, $ M_1^2$, $ M_1M_4$, $ M_1M_7$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_4^2$, $ M_4M_7$, $ M_7^2$, $ \phi_1q_1\tilde{q}_1$, $ M_1\phi_1^2$, $ M_4\phi_1^2$, $ M_7\phi_1^2$, $ q_1\tilde{q}_2$, $ M_1M_2$, $ \phi_1^4$, $ \phi_1q_2\tilde{q}_2$, $ M_2M_4$, $ M_2M_7$, $ \phi_1q_1q_2$, $ M_1M_6$, $ M_4M_6$, $ M_6M_7$, $ M_2\phi_1^2$, $ M_6\phi_1^2$, $ M_1X_1$, $ M_2^2$, $ M_4X_1$, $ M_7X_1$, $ M_2M_6$, $ M_4\phi_1q_2\tilde{q}_1$, $ M_7\phi_1q_2\tilde{q}_1$, $ \phi_1^2X_1$ | $\phi_1^3q_2\tilde{q}_1$ | -1 | t^2.2 + 2*t^2.27 + t^2.49 + t^2.78 + t^3. + t^3.29 + t^3.51 + t^4.02 + t^4.39 + 2*t^4.46 + 3*t^4.54 + t^4.69 + 3*t^4.76 + 2*t^4.98 + 2*t^5.05 + t^5.2 + 3*t^5.27 + t^5.49 + 3*t^5.56 + 3*t^5.78 - t^6. + t^6.07 + 3*t^6.29 + t^6.58 + t^6.59 + 2*t^6.66 + t^6.73 + 5*t^6.8 + t^6.88 + 2*t^6.95 + 3*t^7.02 + 2*t^7.17 + 2*t^7.24 + 3*t^7.31 + t^7.39 + 3*t^7.46 + 5*t^7.54 + t^7.69 + 3*t^7.76 + 5*t^7.83 + 7*t^8.05 - 2*t^8.2 - 2*t^8.27 + 3*t^8.34 - 2*t^8.49 + 5*t^8.56 - 2*t^8.71 - 2*t^8.78 + t^8.79 + 3*t^8.85 + 2*t^8.86 + t^8.93 - t^4.24/y - t^6.44/y - t^6.51/y - t^6.73/y - t^7.02/y + (3*t^7.46)/y + t^7.54/y + t^7.69/y + (3*t^7.76)/y + (2*t^7.98)/y + (3*t^8.05)/y + t^8.2/y + (3*t^8.27)/y + (2*t^8.49)/y + (2*t^8.56)/y - t^8.64/y + (3*t^8.78)/y - t^8.93/y - t^4.24*y - t^6.44*y - t^6.51*y - t^6.73*y - t^7.02*y + 3*t^7.46*y + t^7.54*y + t^7.69*y + 3*t^7.76*y + 2*t^7.98*y + 3*t^8.05*y + t^8.2*y + 3*t^8.27*y + 2*t^8.49*y + 2*t^8.56*y - t^8.64*y + 3*t^8.78*y - t^8.93*y | t^2.2/g1^18 + 2*g1^6*t^2.27 + t^2.49/g1^4 + g1^10*t^2.78 + t^3. + g1^14*t^3.29 + g1^4*t^3.51 + g1^8*t^4.02 + t^4.39/g1^36 + (2*t^4.46)/g1^12 + 3*g1^12*t^4.54 + t^4.69/g1^22 + 3*g1^2*t^4.76 + (2*t^4.98)/g1^8 + 2*g1^16*t^5.05 + t^5.2/g1^18 + 3*g1^6*t^5.27 + t^5.49/g1^4 + 3*g1^20*t^5.56 + 3*g1^10*t^5.78 - t^6. + g1^24*t^6.07 + 3*g1^14*t^6.29 + g1^28*t^6.58 + t^6.59/g1^54 + (2*t^6.66)/g1^30 + t^6.73/g1^6 + 5*g1^18*t^6.8 + t^6.88/g1^40 + (2*t^6.95)/g1^16 + 3*g1^8*t^7.02 + (2*t^7.17)/g1^26 + (2*t^7.24)/g1^2 + 3*g1^22*t^7.31 + t^7.39/g1^36 + (3*t^7.46)/g1^12 + 5*g1^12*t^7.54 + t^7.69/g1^22 + 3*g1^2*t^7.76 + 5*g1^26*t^7.83 + 7*g1^16*t^8.05 - (2*t^8.2)/g1^18 - 2*g1^6*t^8.27 + 3*g1^30*t^8.34 - (2*t^8.49)/g1^4 + 5*g1^20*t^8.56 - (2*t^8.71)/g1^14 - 2*g1^10*t^8.78 + t^8.79/g1^72 + 3*g1^34*t^8.85 + (2*t^8.86)/g1^48 + t^8.93/g1^24 - t^4.24/(g1^2*y) - t^6.44/(g1^20*y) - (g1^4*t^6.51)/y - t^6.73/(g1^6*y) - (g1^8*t^7.02)/y + (3*t^7.46)/(g1^12*y) + (g1^12*t^7.54)/y + t^7.69/(g1^22*y) + (3*g1^2*t^7.76)/y + (2*t^7.98)/(g1^8*y) + (3*g1^16*t^8.05)/y + t^8.2/(g1^18*y) + (3*g1^6*t^8.27)/y + (2*t^8.49)/(g1^4*y) + (2*g1^20*t^8.56)/y - t^8.64/(g1^38*y) + (3*g1^10*t^8.78)/y - t^8.93/(g1^24*y) - (t^4.24*y)/g1^2 - (t^6.44*y)/g1^20 - g1^4*t^6.51*y - (t^6.73*y)/g1^6 - g1^8*t^7.02*y + (3*t^7.46*y)/g1^12 + g1^12*t^7.54*y + (t^7.69*y)/g1^22 + 3*g1^2*t^7.76*y + (2*t^7.98*y)/g1^8 + 3*g1^16*t^8.05*y + (t^8.2*y)/g1^18 + 3*g1^6*t^8.27*y + (2*t^8.49*y)/g1^4 + 2*g1^20*t^8.56*y - (t^8.64*y)/g1^38 + 3*g1^10*t^8.78*y - (t^8.93*y)/g1^24 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 3400 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1q_1\tilde{q}_2$ + $ M_6\phi_1\tilde{q}_1^2$ + $ M_3X_1$ + $ M_5M_7$ | 0.6702 | 0.8472 | 0.7911 | [X:[1.307], M:[0.7557, 0.7831, 0.693, 0.8459, 1.1541, 0.7067, 0.8459], q:[0.8527, 0.3916], qb:[0.4543, 0.7626], phi:[0.3847]] | t^2.12 + t^2.27 + t^2.31 + t^2.35 + 2*t^2.54 + t^3.5 + t^3.69 + t^3.92 + t^4.24 + t^4.39 + t^4.43 + t^4.47 + t^4.53 + t^4.58 + 2*t^4.62 + 3*t^4.66 + t^4.7 + 2*t^4.8 + 3*t^4.85 + 2*t^4.89 + 3*t^5.08 + t^5.62 + t^5.81 + t^5.85 - 2*t^6. - t^4.15/y - t^4.15*y | detail |