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 |
|---|---|---|---|---|---|---|---|---|---|
| 2062 | 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_1M_3$ + $ M_3M_5$ + $ M_2\phi_1^2$ + $ M_6\phi_1^2$ + $ \phi_1\tilde{q}_2^2$ | 0.5606 | 0.728 | 0.77 | [X:[], M:[0.8468, 1.0511, 1.1532, 0.7447, 0.8468, 1.0511], q:[0.6607, 0.4925], qb:[0.1862, 0.7628], phi:[0.4745]] | [X:[], M:[[-12], [4], [12], [-20], [-12], [4]], q:[[-7], [19]], qb:[[-5], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $q_2\tilde{q}_1$, $ M_4$, $ M_1$, $ M_5$, $ \phi_1\tilde{q}_1^2$, $ M_2$, $ M_6$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ M_4q_2\tilde{q}_1$, $ q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2$, $ M_4^2$, $ M_5q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_1^3$, $ M_1M_4$, $ M_4M_5$, $ M_4\phi_1\tilde{q}_1^2$, $ \phi_1q_1q_2$, $ M_1^2$, $ M_1M_5$, $ M_5^2$, $ M_1\phi_1\tilde{q}_1^2$, $ M_5\phi_1\tilde{q}_1^2$, $ \phi_1^2\tilde{q}_1^4$, $ M_6q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ M_2M_4$, $ M_4M_6$, $ \phi_1q_1^2$, $ M_1M_2$, $ M_2M_5$, $ M_1M_6$, $ M_5M_6$, $ M_4\phi_1q_2\tilde{q}_1$, $ M_6\phi_1\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_2$ | $M_5\phi_1q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1^3$ | -1 | t^2.04 + t^2.23 + 3*t^2.54 + 2*t^3.15 + t^3.46 + t^3.96 + t^4.07 + 2*t^4.27 + t^4.38 + t^4.47 + 2*t^4.58 + 3*t^4.77 + t^4.88 + 5*t^5.08 + 2*t^5.19 + 3*t^5.39 + 5*t^5.69 - t^6. + t^6.11 + t^6.2 + 2*t^6.31 + t^6.41 + 3*t^6.5 + 3*t^6.61 + t^6.7 + 3*t^6.81 + t^6.92 + 3*t^7.01 + 3*t^7.12 + t^7.23 + 5*t^7.32 + 3*t^7.42 + t^7.53 + 10*t^7.62 + t^7.84 + 7*t^7.93 - 2*t^8.04 + t^8.14 + 3*t^8.23 + 2*t^8.34 + t^8.43 + t^8.45 - 3*t^8.54 + t^8.65 + 3*t^8.74 + t^8.76 + 2*t^8.85 + t^8.94 - t^4.42/y - t^6.66/y - t^6.96/y + (2*t^7.27)/y + (2*t^7.58)/y + (3*t^7.77)/y + t^7.88/y + (3*t^8.08)/y + (3*t^8.19)/y + (2*t^8.39)/y + t^8.5/y + (7*t^8.69)/y - t^8.89/y - t^4.42*y - t^6.66*y - t^6.96*y + 2*t^7.27*y + 2*t^7.58*y + 3*t^7.77*y + t^7.88*y + 3*t^8.08*y + 3*t^8.19*y + 2*t^8.39*y + t^8.5*y + 7*t^8.69*y - t^8.89*y | g1^14*t^2.04 + t^2.23/g1^20 + (3*t^2.54)/g1^12 + 2*g1^4*t^3.15 + g1^12*t^3.46 + t^3.96/g1^14 + g1^28*t^4.07 + (2*t^4.27)/g1^6 + g1^36*t^4.38 + t^4.47/g1^40 + 2*g1^2*t^4.58 + (3*t^4.77)/g1^32 + g1^10*t^4.88 + (5*t^5.08)/g1^24 + 2*g1^18*t^5.19 + (3*t^5.39)/g1^16 + (5*t^5.69)/g1^8 - t^6. + g1^42*t^6.11 + t^6.2/g1^34 + 2*g1^8*t^6.31 + g1^50*t^6.41 + (3*t^6.5)/g1^26 + 3*g1^16*t^6.61 + t^6.7/g1^60 + (3*t^6.81)/g1^18 + g1^24*t^6.92 + (3*t^7.01)/g1^52 + (3*t^7.12)/g1^10 + g1^32*t^7.23 + (5*t^7.32)/g1^44 + (3*t^7.42)/g1^2 + g1^40*t^7.53 + (10*t^7.62)/g1^36 + g1^48*t^7.84 + (7*t^7.93)/g1^28 - 2*g1^14*t^8.04 + g1^56*t^8.14 + (3*t^8.23)/g1^20 + 2*g1^22*t^8.34 + t^8.43/g1^54 + g1^64*t^8.45 - (3*t^8.54)/g1^12 + g1^30*t^8.65 + (3*t^8.74)/g1^46 + g1^72*t^8.76 + (2*t^8.85)/g1^4 + t^8.94/g1^80 - t^4.42/(g1^2*y) - t^6.66/(g1^22*y) - t^6.96/(g1^14*y) + (2*t^7.27)/(g1^6*y) + (2*g1^2*t^7.58)/y + (3*t^7.77)/(g1^32*y) + (g1^10*t^7.88)/y + (3*t^8.08)/(g1^24*y) + (3*g1^18*t^8.19)/y + (2*t^8.39)/(g1^16*y) + (g1^26*t^8.5)/y + (7*t^8.69)/(g1^8*y) - t^8.89/(g1^42*y) - (t^4.42*y)/g1^2 - (t^6.66*y)/g1^22 - (t^6.96*y)/g1^14 + (2*t^7.27*y)/g1^6 + 2*g1^2*t^7.58*y + (3*t^7.77*y)/g1^32 + g1^10*t^7.88*y + (3*t^8.08*y)/g1^24 + 3*g1^18*t^8.19*y + (2*t^8.39*y)/g1^16 + g1^26*t^8.5*y + (7*t^8.69*y)/g1^8 - (t^8.89*y)/g1^42 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 900 | 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_1M_3$ + $ M_3M_5$ + $ M_2\phi_1^2$ + $ M_6\phi_1^2$ | 0.7013 | 0.8625 | 0.8131 | [X:[], M:[0.9319, 1.0227, 1.0681, 0.8864, 0.9319, 1.0227], q:[0.4865, 0.5816], qb:[0.4453, 0.532], phi:[0.4886]] | t^2.66 + 2*t^2.8 + t^3.06 + 2*t^3.07 + t^3.08 + t^4.14 + t^4.26 + t^4.39 + t^4.4 + t^4.52 + t^4.55 + t^4.66 + t^4.67 + t^4.81 + t^4.96 + t^5.32 + 2*t^5.45 + 2*t^5.59 + 2*t^5.73 + t^5.85 + 3*t^5.86 + t^5.88 - 4*t^6. - t^4.47/y - t^4.47*y | detail |