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 |
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56346 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1\tilde{q}_2^2$ + $ M_6\phi_1q_2^2$ + $ M_1M_7$ | 0.6633 | 0.8362 | 0.7932 | [X:[], M:[1.1968, 1.0521, 0.8032, 0.8756, 1.1244, 0.7873, 0.8032], q:[0.4378, 0.3654], qb:[0.5102, 0.759], phi:[0.4819]] | [X:[], M:[[10], [-38], [-10], [14], [-14], [40], [-10]], q:[[7], [-17]], qb:[[31], [3]], phi:[[-6]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_6$, $ M_3$, $ M_7$, $ M_4$, $ \phi_1^2$, $ M_2$, $ M_5$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_1q_2$, $ \phi_1q_1^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ M_6^2$, $ M_3M_6$, $ M_6M_7$, $ M_3^2$, $ M_3M_7$, $ M_7^2$, $ \phi_1q_2\tilde{q}_2$, $ M_4M_6$, $ M_3M_4$, $ M_4M_7$, $ \phi_1q_1\tilde{q}_2$, $ M_4^2$, $ M_6\phi_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_3\phi_1^2$, $ M_7\phi_1^2$, $ M_2M_6$, $ M_4\phi_1^2$, $ M_2M_3$, $ M_2M_7$, $ M_5M_6$, $ M_2M_4$, $ M_3M_5$, $ M_5M_7$, $ \phi_1^4$ | . | -2 | t^2.36 + 2*t^2.41 + t^2.63 + t^2.89 + t^3.16 + t^3.37 + t^3.81 + t^3.86 + 2*t^4.07 + t^4.29 + t^4.51 + t^4.72 + 2*t^4.77 + 3*t^4.82 + t^4.99 + 2*t^5.04 + 2*t^5.25 + 2*t^5.3 + 2*t^5.52 + t^5.57 + t^5.74 + 2*t^5.78 - 2*t^6. + t^6.05 + t^6.17 + 2*t^6.26 + t^6.31 + 2*t^6.43 + 3*t^6.48 + t^6.53 + t^6.65 + 3*t^6.7 + t^6.87 + 2*t^6.92 + t^6.96 + t^7.09 + 3*t^7.13 + 2*t^7.18 + 4*t^7.23 + t^7.35 + 2*t^7.4 + 2*t^7.45 + 2*t^7.62 + 3*t^7.66 + 3*t^7.71 + 3*t^7.88 + 3*t^7.93 + t^7.98 + t^8.1 + 4*t^8.14 + 2*t^8.19 + t^8.31 - t^8.36 - 3*t^8.41 + t^8.46 + t^8.53 + 2*t^8.58 - 3*t^8.63 + 4*t^8.67 + t^8.72 + 3*t^8.8 + 2*t^8.89 + 2*t^8.94 - t^4.45/y - t^6.81/y - t^6.86/y + t^7.29/y - t^7.34/y + t^7.55/y - t^7.6/y + (2*t^7.77)/y + t^7.82/y + t^7.99/y + (3*t^8.04)/y + t^8.08/y + t^8.25/y + (2*t^8.3)/y + (2*t^8.52)/y + (2*t^8.57)/y + t^8.74/y + (3*t^8.78)/y - t^4.45*y - t^6.81*y - t^6.86*y + t^7.29*y - t^7.34*y + t^7.55*y - t^7.6*y + 2*t^7.77*y + t^7.82*y + t^7.99*y + 3*t^8.04*y + t^8.08*y + t^8.25*y + 2*t^8.3*y + 2*t^8.52*y + 2*t^8.57*y + t^8.74*y + 3*t^8.78*y | g1^40*t^2.36 + (2*t^2.41)/g1^10 + g1^14*t^2.63 + t^2.89/g1^12 + t^3.16/g1^38 + t^3.37/g1^14 + g1^34*t^3.81 + t^3.86/g1^16 + 2*g1^8*t^4.07 + g1^32*t^4.29 + g1^56*t^4.51 + g1^80*t^4.72 + 2*g1^30*t^4.77 + (3*t^4.82)/g1^20 + g1^54*t^4.99 + 2*g1^4*t^5.04 + 2*g1^28*t^5.25 + (2*t^5.3)/g1^22 + 2*g1^2*t^5.52 + t^5.57/g1^48 + g1^26*t^5.74 + (2*t^5.78)/g1^24 - 2*t^6. + t^6.05/g1^50 + g1^74*t^6.17 + (2*t^6.26)/g1^26 + t^6.31/g1^76 + 2*g1^48*t^6.43 + (3*t^6.48)/g1^2 + t^6.53/g1^52 + g1^72*t^6.65 + 3*g1^22*t^6.7 + g1^96*t^6.87 + 2*g1^46*t^6.92 + t^6.96/g1^4 + g1^120*t^7.09 + 3*g1^70*t^7.13 + 2*g1^20*t^7.18 + (4*t^7.23)/g1^30 + g1^94*t^7.35 + 2*g1^44*t^7.4 + (2*t^7.45)/g1^6 + 2*g1^68*t^7.62 + 3*g1^18*t^7.66 + (3*t^7.71)/g1^32 + 3*g1^42*t^7.88 + (3*t^7.93)/g1^8 + t^7.98/g1^58 + g1^66*t^8.1 + 4*g1^16*t^8.14 + (2*t^8.19)/g1^34 + g1^90*t^8.31 - g1^40*t^8.36 - (3*t^8.41)/g1^10 + t^8.46/g1^60 + g1^114*t^8.53 + 2*g1^64*t^8.58 - 3*g1^14*t^8.63 + (4*t^8.67)/g1^36 + t^8.72/g1^86 + 3*g1^88*t^8.8 + (2*t^8.89)/g1^12 + (2*t^8.94)/g1^62 - t^4.45/(g1^6*y) - (g1^34*t^6.81)/y - t^6.86/(g1^16*y) + (g1^32*t^7.29)/y - t^7.34/(g1^18*y) + (g1^6*t^7.55)/y - t^7.6/(g1^44*y) + (2*g1^30*t^7.77)/y + t^7.82/(g1^20*y) + (g1^54*t^7.99)/y + (3*g1^4*t^8.04)/y + t^8.08/(g1^46*y) + (g1^28*t^8.25)/y + (2*t^8.3)/(g1^22*y) + (2*g1^2*t^8.52)/y + (2*t^8.57)/(g1^48*y) + (g1^26*t^8.74)/y + (3*t^8.78)/(g1^24*y) - (t^4.45*y)/g1^6 - g1^34*t^6.81*y - (t^6.86*y)/g1^16 + g1^32*t^7.29*y - (t^7.34*y)/g1^18 + g1^6*t^7.55*y - (t^7.6*y)/g1^44 + 2*g1^30*t^7.77*y + (t^7.82*y)/g1^20 + g1^54*t^7.99*y + 3*g1^4*t^8.04*y + (t^8.08*y)/g1^46 + g1^28*t^8.25*y + (2*t^8.3*y)/g1^22 + 2*g1^2*t^8.52*y + (2*t^8.57*y)/g1^48 + g1^26*t^8.74*y + (3*t^8.78*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 |
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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 |
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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 |
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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 |
---|---|---|---|---|---|---|---|---|---|
52426 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1\tilde{q}_2^2$ + $ M_6\phi_1q_2^2$ | 0.6471 | 0.8081 | 0.8007 | [X:[], M:[1.1947, 1.0602, 0.8053, 0.8726, 1.1274, 0.7788], q:[0.4363, 0.369], qb:[0.5035, 0.7584], phi:[0.4832]] | t^2.34 + t^2.42 + t^2.62 + t^2.9 + t^3.18 + t^3.38 + t^3.58 + t^3.79 + t^3.87 + 2*t^4.07 + t^4.27 + t^4.47 + t^4.67 + t^4.75 + t^4.83 + t^4.95 + t^5.03 + 2*t^5.24 + t^5.32 + 2*t^5.52 + t^5.72 + t^5.8 + t^5.92 - t^6. - t^4.45/y - t^4.45*y | detail |