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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56479 | 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\tilde{q}_1\tilde{q}_2$ + $ M_5M_7$ | 0.6611 | 0.834 | 0.7927 | [X:[], M:[1.2024, 1.0309, 0.7976, 0.8833, 1.1167, 0.7119, 0.8833], q:[0.4417, 0.3559], qb:[0.5274, 0.7607], phi:[0.4786]] | [X:[], M:[[10], [-38], [-10], [14], [-14], [-34], [14]], 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_4$, $ M_7$, $ \phi_1^2$, $ M_2$, $ \phi_1q_2^2$, $ M_1$, $ \phi_1q_1q_2$, $ \phi_1q_1^2$, $ \phi_1q_2\tilde{q}_1$, $ M_6^2$, $ \phi_1q_1\tilde{q}_1$, $ M_3M_6$, $ \phi_1\tilde{q}_1^2$, $ M_3^2$, $ M_4M_6$, $ M_6M_7$, $ \phi_1q_2\tilde{q}_2$, $ M_6\phi_1^2$, $ M_3M_4$, $ M_3M_7$, $ \phi_1q_1\tilde{q}_2$, $ M_2M_6$, $ M_3\phi_1^2$, $ M_4^2$, $ M_4M_7$, $ M_7^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_4\phi_1^2$, $ M_7\phi_1^2$, $ M_6\phi_1q_2^2$, $ M_2M_4$, $ M_1M_6$, $ M_2M_7$, $ \phi_1^4$, $ M_2\phi_1^2$, $ M_6\phi_1q_1q_2$, $ M_3\phi_1q_2^2$ | . | -2 | t^2.14 + t^2.39 + 2*t^2.65 + t^2.87 + t^3.09 + t^3.57 + t^3.61 + t^3.83 + 2*t^4.09 + t^4.27 + t^4.34 + t^4.53 + t^4.6 + 3*t^4.79 + t^5.01 + 2*t^5.04 + t^5.23 + t^5.26 + 3*t^5.3 + 2*t^5.52 + t^5.71 + 2*t^5.74 + 3*t^5.96 - 2*t^6. + t^6.19 + 4*t^6.22 - t^6.26 + t^6.41 + t^6.44 + 4*t^6.48 - t^6.51 + 2*t^6.66 + 4*t^6.74 + 3*t^6.92 + 2*t^6.99 + 2*t^7.14 + 3*t^7.18 - t^7.21 + 2*t^7.25 + t^7.36 + 2*t^7.4 + 3*t^7.44 + 5*t^7.66 + 2*t^7.69 - t^7.73 + t^7.84 + 2*t^7.88 + 3*t^7.91 + 2*t^7.95 + 3*t^8.1 - 3*t^8.14 + 5*t^8.17 + t^8.32 + 5*t^8.36 - 2*t^8.39 + t^8.43 + t^8.54 + t^8.58 + 7*t^8.61 - 8*t^8.65 + 2*t^8.69 + 2*t^8.8 + 3*t^8.84 + 5*t^8.87 - 4*t^8.91 + t^8.94 - t^4.44/y - t^6.57/y - t^7.09/y - t^7.31/y + t^7.34/y + t^7.56/y + (3*t^7.79)/y + t^8.01/y + (2*t^8.04)/y + t^8.23/y + t^8.26/y + (2*t^8.3)/y + t^8.49/y + (2*t^8.52)/y + (3*t^8.74)/y + (3*t^8.96)/y - t^4.44*y - t^6.57*y - t^7.09*y - t^7.31*y + t^7.34*y + t^7.56*y + 3*t^7.79*y + t^8.01*y + 2*t^8.04*y + t^8.23*y + t^8.26*y + 2*t^8.3*y + t^8.49*y + 2*t^8.52*y + 3*t^8.74*y + 3*t^8.96*y | t^2.14/g1^34 + t^2.39/g1^10 + 2*g1^14*t^2.65 + t^2.87/g1^12 + t^3.09/g1^38 + t^3.57/g1^40 + g1^10*t^3.61 + t^3.83/g1^16 + 2*g1^8*t^4.09 + t^4.27/g1^68 + g1^32*t^4.34 + t^4.53/g1^44 + g1^56*t^4.6 + (3*t^4.79)/g1^20 + t^5.01/g1^46 + 2*g1^4*t^5.04 + t^5.23/g1^72 + t^5.26/g1^22 + 3*g1^28*t^5.3 + 2*g1^2*t^5.52 + t^5.71/g1^74 + (2*t^5.74)/g1^24 + (3*t^5.96)/g1^50 - 2*t^6. + t^6.19/g1^76 + (4*t^6.22)/g1^26 - g1^24*t^6.26 + t^6.41/g1^102 + t^6.44/g1^52 + (4*t^6.48)/g1^2 - g1^48*t^6.51 + (2*t^6.66)/g1^78 + 4*g1^22*t^6.74 + (3*t^6.92)/g1^54 + 2*g1^46*t^6.99 + (2*t^7.14)/g1^80 + (3*t^7.18)/g1^30 - g1^20*t^7.21 + 2*g1^70*t^7.25 + t^7.36/g1^106 + (2*t^7.4)/g1^56 + (3*t^7.44)/g1^6 + (5*t^7.66)/g1^32 + 2*g1^18*t^7.69 - g1^68*t^7.73 + t^7.84/g1^108 + (2*t^7.88)/g1^58 + (3*t^7.91)/g1^8 + 2*g1^42*t^7.95 + (3*t^8.1)/g1^84 - (3*t^8.14)/g1^34 + 5*g1^16*t^8.17 + t^8.32/g1^110 + (5*t^8.36)/g1^60 - (2*t^8.39)/g1^10 + g1^40*t^8.43 + t^8.54/g1^136 + t^8.58/g1^86 + (7*t^8.61)/g1^36 - 8*g1^14*t^8.65 + 2*g1^64*t^8.69 + (2*t^8.8)/g1^112 + (3*t^8.84)/g1^62 + (5*t^8.87)/g1^12 - 4*g1^38*t^8.91 + g1^88*t^8.94 - t^4.44/(g1^6*y) - t^6.57/(g1^40*y) - (g1^8*t^7.09)/y - t^7.31/(g1^18*y) + (g1^32*t^7.34)/y + (g1^6*t^7.56)/y + (3*t^7.79)/(g1^20*y) + t^8.01/(g1^46*y) + (2*g1^4*t^8.04)/y + t^8.23/(g1^72*y) + t^8.26/(g1^22*y) + (2*g1^28*t^8.3)/y + t^8.49/(g1^48*y) + (2*g1^2*t^8.52)/y + (3*t^8.74)/(g1^24*y) + (3*t^8.96)/(g1^50*y) - (t^4.44*y)/g1^6 - (t^6.57*y)/g1^40 - g1^8*t^7.09*y - (t^7.31*y)/g1^18 + g1^32*t^7.34*y + g1^6*t^7.56*y + (3*t^7.79*y)/g1^20 + (t^8.01*y)/g1^46 + 2*g1^4*t^8.04*y + (t^8.23*y)/g1^72 + (t^8.26*y)/g1^22 + 2*g1^28*t^8.3*y + (t^8.49*y)/g1^48 + 2*g1^2*t^8.52*y + (3*t^8.74*y)/g1^24 + (3*t^8.96*y)/g1^50 |
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 |
---|---|---|---|---|---|---|---|---|---|
53808 | 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\tilde{q}_1\tilde{q}_2$ | 0.6508 | 0.8175 | 0.7961 | [X:[], M:[1.2064, 1.0156, 0.7936, 0.889, 1.111, 0.6982], q:[0.4445, 0.3491], qb:[0.5399, 0.7619], phi:[0.4761]] | t^2.09 + t^2.38 + t^2.67 + t^2.86 + t^3.05 + t^3.33 + t^3.52 + t^3.62 + t^3.81 + 2*t^4.1 + t^4.19 + t^4.38 + t^4.48 + t^4.67 + 2*t^4.76 + t^4.95 + t^5.05 + t^5.14 + t^5.24 + t^5.33 + t^5.43 + t^5.52 + t^5.62 + 2*t^5.71 + 3*t^5.9 - t^6. - t^4.43/y - t^4.43*y | detail |