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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56730 | 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$ + $ \phi_1\tilde{q}_2^2$ + $ M_6\phi_1q_1q_2$ + $ M_5\phi_1^2$ + $ M_7\phi_1q_1^2$ | 0.6894 | 0.8769 | 0.7862 | [X:[], M:[1.1701, 1.0747, 0.8299, 0.8119, 1.0567, 0.6985, 0.7164], q:[0.406, 0.4239], qb:[0.5194, 0.7642], phi:[0.4716]] | [X:[], M:[[12], [-30], [-12], [22], [4], [14], [-20]], q:[[11], [-23]], qb:[[19], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_6$, $ M_7$, $ M_4$, $ M_3$, $ \phi_1^2$, $ M_5$, $ M_2$, $ M_1$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2$, $ M_6^2$, $ \phi_1q_1\tilde{q}_1$, $ M_6M_7$, $ \phi_1q_2\tilde{q}_1$, $ M_7^2$, $ M_4M_6$, $ \phi_1\tilde{q}_1^2$, $ M_3M_6$, $ M_4M_7$, $ M_3M_7$, $ M_4^2$, $ M_3M_4$, $ M_6\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ M_3^2$, $ M_7\phi_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_5M_6$, $ M_4\phi_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_2M_6$, $ M_5M_7$, $ M_3\phi_1^2$, $ M_2M_7$, $ M_4M_5$, $ M_1M_6$, $ M_2M_4$, $ M_3M_5$, $ M_1M_7$, $ \phi_1^4$, $ M_1M_4$, $ M_6\tilde{q}_1\tilde{q}_2$ | $M_7\tilde{q}_1\tilde{q}_2$ | 0 | t^2.1 + t^2.15 + t^2.44 + t^2.49 + t^2.83 + t^3.17 + t^3.22 + t^3.51 + t^3.85 + t^3.96 + 2*t^4.19 + 2*t^4.24 + t^4.3 + 2*t^4.53 + 2*t^4.59 + t^4.64 + t^4.87 + 2*t^4.93 + 2*t^4.98 + 2*t^5.27 + 3*t^5.32 + t^5.37 + 2*t^5.61 + 3*t^5.66 + t^5.95 + t^6.05 + t^6.11 + 2*t^6.29 + 3*t^6.34 + 3*t^6.39 + 3*t^6.45 + 3*t^6.63 + 5*t^6.68 + 2*t^6.73 + 2*t^6.79 + 2*t^6.97 + 4*t^7.02 + 2*t^7.07 + t^7.13 + t^7.18 + t^7.31 + 4*t^7.36 + 3*t^7.41 + 4*t^7.47 + t^7.52 + 3*t^7.7 + 4*t^7.76 + 3*t^7.81 + t^7.92 + 3*t^8.04 + t^8.15 + 2*t^8.2 + t^8.26 + 3*t^8.38 + 4*t^8.49 + 4*t^8.54 + 3*t^8.6 + 4*t^8.72 + 5*t^8.78 + 3*t^8.83 + 4*t^8.88 + 3*t^8.94 - t^4.41/y - t^6.51/y - t^6.56/y - t^6.85/y + t^7.19/y + t^7.24/y + t^7.53/y + (2*t^7.59)/y + (2*t^7.93)/y + (2*t^7.98)/y + (3*t^8.27)/y + (4*t^8.32)/y + t^8.37/y + t^8.61/y + (2*t^8.66)/y + t^8.95/y - t^4.41*y - t^6.51*y - t^6.56*y - t^6.85*y + t^7.19*y + t^7.24*y + t^7.53*y + 2*t^7.59*y + 2*t^7.93*y + 2*t^7.98*y + 3*t^8.27*y + 4*t^8.32*y + t^8.37*y + t^8.61*y + 2*t^8.66*y + t^8.95*y | g1^14*t^2.1 + t^2.15/g1^20 + g1^22*t^2.44 + t^2.49/g1^12 + t^2.83/g1^4 + g1^4*t^3.17 + t^3.22/g1^30 + g1^12*t^3.51 + g1^20*t^3.85 + t^3.96/g1^48 + 2*g1^28*t^4.19 + (2*t^4.24)/g1^6 + t^4.3/g1^40 + 2*g1^36*t^4.53 + 2*g1^2*t^4.59 + t^4.64/g1^32 + g1^44*t^4.87 + 2*g1^10*t^4.93 + (2*t^4.98)/g1^24 + 2*g1^18*t^5.27 + (3*t^5.32)/g1^16 + t^5.37/g1^50 + 2*g1^26*t^5.61 + (3*t^5.66)/g1^8 + g1^34*t^5.95 + t^6.05/g1^34 + t^6.11/g1^68 + 2*g1^42*t^6.29 + 3*g1^8*t^6.34 + (3*t^6.39)/g1^26 + (3*t^6.45)/g1^60 + 3*g1^50*t^6.63 + 5*g1^16*t^6.68 + (2*t^6.73)/g1^18 + (2*t^6.79)/g1^52 + 2*g1^58*t^6.97 + 4*g1^24*t^7.02 + (2*t^7.07)/g1^10 + t^7.13/g1^44 + t^7.18/g1^78 + g1^66*t^7.31 + 4*g1^32*t^7.36 + (3*t^7.41)/g1^2 + (4*t^7.47)/g1^36 + t^7.52/g1^70 + 3*g1^40*t^7.7 + 4*g1^6*t^7.76 + (3*t^7.81)/g1^28 + t^7.92/g1^96 + 3*g1^48*t^8.04 + t^8.15/g1^20 + (2*t^8.2)/g1^54 + t^8.26/g1^88 + 3*g1^56*t^8.38 + (4*t^8.49)/g1^12 + (4*t^8.54)/g1^46 + (3*t^8.6)/g1^80 + 4*g1^64*t^8.72 + 5*g1^30*t^8.78 + (3*t^8.83)/g1^4 + (4*t^8.88)/g1^38 + (3*t^8.94)/g1^72 - t^4.41/(g1^2*y) - (g1^12*t^6.51)/y - t^6.56/(g1^22*y) - (g1^20*t^6.85)/y + (g1^28*t^7.19)/y + t^7.24/(g1^6*y) + (g1^36*t^7.53)/y + (2*g1^2*t^7.59)/y + (2*g1^10*t^7.93)/y + (2*t^7.98)/(g1^24*y) + (3*g1^18*t^8.27)/y + (4*t^8.32)/(g1^16*y) + t^8.37/(g1^50*y) + (g1^26*t^8.61)/y + (2*t^8.66)/(g1^8*y) + (g1^34*t^8.95)/y - (t^4.41*y)/g1^2 - g1^12*t^6.51*y - (t^6.56*y)/g1^22 - g1^20*t^6.85*y + g1^28*t^7.19*y + (t^7.24*y)/g1^6 + g1^36*t^7.53*y + 2*g1^2*t^7.59*y + 2*g1^10*t^7.93*y + (2*t^7.98*y)/g1^24 + 3*g1^18*t^8.27*y + (4*t^8.32*y)/g1^16 + (t^8.37*y)/g1^50 + g1^26*t^8.61*y + (2*t^8.66*y)/g1^8 + g1^34*t^8.95*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 |
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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 |
---|---|---|---|---|---|---|---|---|---|
55099 | 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$ + $ \phi_1\tilde{q}_2^2$ + $ M_6\phi_1q_1q_2$ + $ M_5\phi_1^2$ | 0.6693 | 0.8394 | 0.7974 | [X:[], M:[1.167, 1.0824, 0.833, 0.8062, 1.0557, 0.6949], q:[0.4031, 0.4299], qb:[0.5145, 0.7639], phi:[0.4722]] | t^2.08 + t^2.42 + t^2.5 + t^2.83 + t^3.17 + t^3.25 + t^3.5 + 2*t^3.84 + t^4. + 2*t^4.17 + t^4.25 + 2*t^4.5 + t^4.58 + t^4.84 + 2*t^4.92 + t^5. + 2*t^5.25 + 2*t^5.33 + 2*t^5.59 + 2*t^5.67 + 2*t^5.92 - t^6. - t^4.42/y - t^4.42*y | detail |