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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55422 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_1\phi_1^2$ + $ M_3\phi_1q_2^2$ + $ M_1M_4$ + $ M_3M_5$ + $ M_6\phi_1\tilde{q}_2^2$ | 0.6287 | 0.825 | 0.7621 | [X:[], M:[0.9533, 0.8033, 0.86, 1.0467, 1.14, 0.6733], q:[0.7383, 0.3083], qb:[0.4583, 0.4017], phi:[0.5233]] | [X:[], M:[[-4], [26], [-12], [4], [12], [-28]], q:[[-1], [5]], qb:[[-25], [13]], phi:[[2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_6$, $ q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ M_2$, $ \tilde{q}_1\tilde{q}_2$, $ M_4$, $ \phi_1^2$, $ M_5$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ M_6^2$, $ M_6q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_6q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ M_2M_6$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ M_2q_2\tilde{q}_2$, $ q_2^2\tilde{q}_1^2$, $ M_6\tilde{q}_1\tilde{q}_2$, $ \phi_1q_1q_2$, $ M_2q_2\tilde{q}_1$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ M_2^2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ \phi_1q_1\tilde{q}_2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ M_4M_6$, $ M_6\phi_1^2$, $ \phi_1q_1\tilde{q}_1$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_4q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_5M_6$, $ M_6\phi_1q_2^2$, $ M_4q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_2M_4$, $ M_2\phi_1^2$, $ M_5q_2\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_5q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_1$, $ M_6\phi_1q_2\tilde{q}_2$, $ M_4\tilde{q}_1\tilde{q}_2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ M_2M_5$, $ M_2\phi_1q_2^2$, $ \phi_1q_2^2\tilde{q}_2^2$, $ M_6\phi_1q_2\tilde{q}_1$ | $M_5\tilde{q}_1\tilde{q}_2$, $ 2\phi_1q_2^2\tilde{q}_1\tilde{q}_2$ | 0 | t^2.02 + t^2.13 + t^2.3 + t^2.41 + t^2.58 + 2*t^3.14 + 2*t^3.42 + t^3.7 + t^3.87 + t^4.04 + 2*t^4.15 + t^4.26 + 2*t^4.32 + 2*t^4.43 + t^4.54 + 2*t^4.6 + 2*t^4.71 + t^4.82 + t^4.88 + t^4.99 + 3*t^5.16 + 2*t^5.27 + 4*t^5.44 + 3*t^5.55 + 3*t^5.72 + 2*t^5.83 + t^5.89 + t^6.06 + t^6.11 + 2*t^6.17 + 3*t^6.28 + 2*t^6.34 + t^6.39 + 3*t^6.45 + 5*t^6.56 + 3*t^6.62 + t^6.67 + 3*t^6.73 + 5*t^6.84 + 3*t^6.9 + t^6.95 + 2*t^7.01 + 2*t^7.12 + 3*t^7.18 + t^7.23 + 4*t^7.29 + 2*t^7.4 + 6*t^7.46 + 4*t^7.57 + 3*t^7.68 + 6*t^7.74 + 3*t^7.85 + t^7.91 + 3*t^7.96 + t^8.02 + t^8.08 + t^8.13 + 3*t^8.19 + 2*t^8.24 + 2*t^8.3 + 2*t^8.36 + t^8.41 + 4*t^8.47 + 2*t^8.52 + 4*t^8.58 + 4*t^8.64 + 4*t^8.69 + 3*t^8.75 + t^8.8 + 5*t^8.86 + 4*t^8.92 + 5*t^8.97 - t^4.57/y - t^6.59/y - t^6.98/y + t^7.15/y + t^7.32/y + (3*t^7.43)/y + t^7.54/y + t^7.6/y + t^7.71/y + t^7.88/y + t^7.99/y + (3*t^8.16)/y + (2*t^8.27)/y + (4*t^8.44)/y + (5*t^8.55)/y - t^8.61/y + (5*t^8.72)/y + (3*t^8.83)/y + t^8.89/y - t^4.57*y - t^6.59*y - t^6.98*y + t^7.15*y + t^7.32*y + 3*t^7.43*y + t^7.54*y + t^7.6*y + t^7.71*y + t^7.88*y + t^7.99*y + 3*t^8.16*y + 2*t^8.27*y + 4*t^8.44*y + 5*t^8.55*y - t^8.61*y + 5*t^8.72*y + 3*t^8.83*y + t^8.89*y | t^2.02/g1^28 + g1^18*t^2.13 + t^2.3/g1^20 + g1^26*t^2.41 + t^2.58/g1^12 + 2*g1^4*t^3.14 + 2*g1^12*t^3.42 + g1^20*t^3.7 + t^3.87/g1^18 + t^4.04/g1^56 + (2*t^4.15)/g1^10 + g1^36*t^4.26 + (2*t^4.32)/g1^48 + (2*t^4.43)/g1^2 + g1^44*t^4.54 + (2*t^4.6)/g1^40 + 2*g1^6*t^4.71 + g1^52*t^4.82 + t^4.88/g1^32 + g1^14*t^4.99 + (3*t^5.16)/g1^24 + 2*g1^22*t^5.27 + (4*t^5.44)/g1^16 + 3*g1^30*t^5.55 + (3*t^5.72)/g1^8 + 2*g1^38*t^5.83 + t^5.89/g1^46 + t^6.06/g1^84 + g1^46*t^6.11 + (2*t^6.17)/g1^38 + 3*g1^8*t^6.28 + (2*t^6.34)/g1^76 + g1^54*t^6.39 + (3*t^6.45)/g1^30 + 5*g1^16*t^6.56 + (3*t^6.62)/g1^68 + g1^62*t^6.67 + (3*t^6.73)/g1^22 + 5*g1^24*t^6.84 + (3*t^6.9)/g1^60 + g1^70*t^6.95 + (2*t^7.01)/g1^14 + 2*g1^32*t^7.12 + (3*t^7.18)/g1^52 + g1^78*t^7.23 + (4*t^7.29)/g1^6 + 2*g1^40*t^7.4 + (6*t^7.46)/g1^44 + 4*g1^2*t^7.57 + 3*g1^48*t^7.68 + (6*t^7.74)/g1^36 + 3*g1^10*t^7.85 + t^7.91/g1^74 + 3*g1^56*t^7.96 + t^8.02/g1^28 + t^8.08/g1^112 + g1^18*t^8.13 + (3*t^8.19)/g1^66 + 2*g1^64*t^8.24 + (2*t^8.3)/g1^20 + (2*t^8.36)/g1^104 + g1^26*t^8.41 + (4*t^8.47)/g1^58 + 2*g1^72*t^8.52 + (4*t^8.58)/g1^12 + (4*t^8.64)/g1^96 + 4*g1^34*t^8.69 + (3*t^8.75)/g1^50 + g1^80*t^8.8 + (5*t^8.86)/g1^4 + (4*t^8.92)/g1^88 + 5*g1^42*t^8.97 - (g1^2*t^4.57)/y - t^6.59/(g1^26*y) - (g1^28*t^6.98)/y + t^7.15/(g1^10*y) + t^7.32/(g1^48*y) + (3*t^7.43)/(g1^2*y) + (g1^44*t^7.54)/y + t^7.6/(g1^40*y) + (g1^6*t^7.71)/y + t^7.88/(g1^32*y) + (g1^14*t^7.99)/y + (3*t^8.16)/(g1^24*y) + (2*g1^22*t^8.27)/y + (4*t^8.44)/(g1^16*y) + (5*g1^30*t^8.55)/y - t^8.61/(g1^54*y) + (5*t^8.72)/(g1^8*y) + (3*g1^38*t^8.83)/y + t^8.89/(g1^46*y) - g1^2*t^4.57*y - (t^6.59*y)/g1^26 - g1^28*t^6.98*y + (t^7.15*y)/g1^10 + (t^7.32*y)/g1^48 + (3*t^7.43*y)/g1^2 + g1^44*t^7.54*y + (t^7.6*y)/g1^40 + g1^6*t^7.71*y + (t^7.88*y)/g1^32 + g1^14*t^7.99*y + (3*t^8.16*y)/g1^24 + 2*g1^22*t^8.27*y + (4*t^8.44*y)/g1^16 + 5*g1^30*t^8.55*y - (t^8.61*y)/g1^54 + (5*t^8.72*y)/g1^8 + 3*g1^38*t^8.83*y + (t^8.89*y)/g1^46 |
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 |
---|---|---|---|---|---|---|---|---|---|
47064 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_1\phi_1^2$ + $ M_3\phi_1q_2^2$ + $ M_1M_4$ + $ M_3M_5$ | 0.6079 | 0.7838 | 0.7756 | [X:[], M:[0.9536, 0.8018, 0.8607, 1.0464, 1.1393], q:[0.7384, 0.308], qb:[0.4598, 0.4009], phi:[0.5232]] | t^2.13 + t^2.3 + t^2.41 + t^2.58 + 2*t^3.14 + 2*t^3.42 + t^3.7 + t^3.87 + t^3.98 + t^4.15 + t^4.25 + t^4.33 + t^4.43 + t^4.53 + t^4.61 + 2*t^4.71 + t^4.81 + t^4.89 + t^4.99 + t^5.16 + 2*t^5.27 + 2*t^5.44 + 3*t^5.54 + 2*t^5.72 + 2*t^5.82 - t^4.57/y - t^4.57*y | detail |