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 |
|---|---|---|---|---|---|---|---|---|---|
| 1259 | SU2adj1nf2 | $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_1^2$ + $ M_2M_5$ + $ M_1M_5$ + $ M_3M_4$ + $ M_5M_6$ | 0.6029 | 0.7691 | 0.7839 | [X:[], M:[0.6807, 0.6807, 1.0639, 0.9361, 1.3193, 0.6807], q:[0.9895, 0.6063], qb:[0.3298, 0.4575], phi:[0.4042]] | [X:[], M:[[-20], [-20], [4], [-4], [20], [-20]], q:[[15], [-9]], qb:[[5], [13]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ M_6$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1^2$, $ M_4$, $ M_3$, $ q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1^2$, $ M_1M_6$, $ M_6^2$, $ q_1\tilde{q}_2$, $ M_1\tilde{q}_1\tilde{q}_2$, $ M_6\tilde{q}_1\tilde{q}_2$, $ M_1\phi_1^2$, $ M_6\phi_1^2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ q_1q_2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ M_1M_4$, $ M_4M_6$, $ \phi_1^4$, $ M_4\tilde{q}_1\tilde{q}_2$, $ M_1M_3$, $ M_3M_6$, $ M_4\phi_1^2$, $ M_1q_2\tilde{q}_2$, $ M_6q_2\tilde{q}_2$, $ M_3\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ M_4^2$, $ M_3\phi_1^2$, $ M_1\phi_1\tilde{q}_1\tilde{q}_2$, $ M_6\phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2\tilde{q}_2^2$ | $M_4q_2\tilde{q}_2$, $ \phi_1^3\tilde{q}_1\tilde{q}_2$ | 0 | 2*t^2.04 + t^2.36 + t^2.43 + t^2.81 + 2*t^3.19 + t^3.57 + 3*t^4.08 + t^4.34 + 2*t^4.4 + 2*t^4.47 + t^4.72 + 2*t^4.79 + 3*t^4.85 + t^5.17 + 4*t^5.23 + 2*t^5.55 + 3*t^5.62 + t^5.94 + 4*t^6.13 + 3*t^6.38 + 2*t^6.45 + 3*t^6.51 + t^6.7 + 2*t^6.77 + 2*t^6.83 + 5*t^6.89 + t^7.09 + t^7.15 + 2*t^7.21 + 7*t^7.28 + t^7.53 + 2*t^7.6 + 5*t^7.66 + 2*t^7.92 + 2*t^7.98 + 5*t^8.17 + t^8.3 - t^8.36 + 3*t^8.43 + 2*t^8.49 + 4*t^8.55 + t^8.68 + t^8.75 - t^8.81 + 2*t^8.87 + 7*t^8.93 - t^4.21/y - (2*t^6.25)/y - t^6.64/y + t^7.08/y + (2*t^7.4)/y + (2*t^7.47)/y + (2*t^7.79)/y + (2*t^7.85)/y + (3*t^8.17)/y + (5*t^8.23)/y - (3*t^8.3)/y + (2*t^8.55)/y + (4*t^8.62)/y - (2*t^8.68)/y + t^8.94/y - t^4.21*y - 2*t^6.25*y - t^6.64*y + t^7.08*y + 2*t^7.4*y + 2*t^7.47*y + 2*t^7.79*y + 2*t^7.85*y + 3*t^8.17*y + 5*t^8.23*y - 3*t^8.3*y + 2*t^8.55*y + 4*t^8.62*y - 2*t^8.68*y + t^8.94*y | (2*t^2.04)/g1^20 + g1^18*t^2.36 + t^2.43/g1^12 + t^2.81/g1^4 + 2*g1^4*t^3.19 + g1^12*t^3.57 + (3*t^4.08)/g1^40 + g1^28*t^4.34 + (2*t^4.4)/g1^2 + (2*t^4.47)/g1^32 + g1^36*t^4.72 + 2*g1^6*t^4.79 + (3*t^4.85)/g1^24 + g1^14*t^5.17 + (4*t^5.23)/g1^16 + 2*g1^22*t^5.55 + (3*t^5.62)/g1^8 + g1^30*t^5.94 + (4*t^6.13)/g1^60 + 3*g1^8*t^6.38 + (2*t^6.45)/g1^22 + (3*t^6.51)/g1^52 + g1^46*t^6.7 + 2*g1^16*t^6.77 + (2*t^6.83)/g1^14 + (5*t^6.89)/g1^44 + g1^54*t^7.09 + g1^24*t^7.15 + (2*t^7.21)/g1^6 + (7*t^7.28)/g1^36 + g1^32*t^7.53 + 2*g1^2*t^7.6 + (5*t^7.66)/g1^28 + 2*g1^40*t^7.92 + 2*g1^10*t^7.98 + (5*t^8.17)/g1^80 + g1^48*t^8.3 - g1^18*t^8.36 + (3*t^8.43)/g1^12 + (2*t^8.49)/g1^42 + (4*t^8.55)/g1^72 + g1^56*t^8.68 + g1^26*t^8.75 - t^8.81/g1^4 + (2*t^8.87)/g1^34 + (7*t^8.93)/g1^64 - t^4.21/(g1^6*y) - (2*t^6.25)/(g1^26*y) - t^6.64/(g1^18*y) + t^7.08/(g1^40*y) + (2*t^7.4)/(g1^2*y) + (2*t^7.47)/(g1^32*y) + (2*g1^6*t^7.79)/y + (2*t^7.85)/(g1^24*y) + (3*g1^14*t^8.17)/y + (5*t^8.23)/(g1^16*y) - (3*t^8.3)/(g1^46*y) + (2*g1^22*t^8.55)/y + (4*t^8.62)/(g1^8*y) - (2*t^8.68)/(g1^38*y) + (g1^30*t^8.94)/y - (t^4.21*y)/g1^6 - (2*t^6.25*y)/g1^26 - (t^6.64*y)/g1^18 + (t^7.08*y)/g1^40 + (2*t^7.4*y)/g1^2 + (2*t^7.47*y)/g1^32 + 2*g1^6*t^7.79*y + (2*t^7.85*y)/g1^24 + 3*g1^14*t^8.17*y + (5*t^8.23*y)/g1^16 - (3*t^8.3*y)/g1^46 + 2*g1^22*t^8.55*y + (4*t^8.62*y)/g1^8 - (2*t^8.68*y)/g1^38 + g1^30*t^8.94*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 |
|---|---|---|---|---|---|---|---|---|---|
| 772 | SU2adj1nf2 | $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_1^2$ + $ M_2M_5$ + $ M_1M_5$ + $ M_3M_4$ | 0.5822 | 0.7285 | 0.7991 | [X:[], M:[0.6846, 0.6846, 1.0631, 0.9369, 1.3154], q:[0.9866, 0.608], qb:[0.3289, 0.455], phi:[0.4054]] | t^2.05 + t^2.35 + t^2.43 + t^2.81 + 2*t^3.19 + t^3.57 + t^3.95 + t^4.11 + t^4.32 + t^4.41 + t^4.49 + t^4.7 + 2*t^4.78 + 2*t^4.86 + t^5.16 + 2*t^5.24 + 2*t^5.54 + 2*t^5.62 + t^5.92 + t^6. - t^4.22/y - t^4.22*y | detail |