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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5851 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_1$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_2\tilde{q}_1$ + $ M_4M_6$ + $ M_1M_5$ + $ M_5M_7$ + $ \phi_1q_1^2$ + $ M_6M_8$ + $ M_9\phi_1q_2\tilde{q}_1$ | 0.6741 | 0.8573 | 0.7863 | [X:[], M:[0.8732, 1.0341, 1.0585, 0.8049, 1.1268, 1.1951, 0.8732, 0.8049, 0.7122], q:[0.7585, 0.3683], qb:[0.4366, 0.5049], phi:[0.4829]] | [X:[], M:[[14], [12], [-38], [-10], [-14], [10], [14], [-10], [16]], q:[[3], [-17]], qb:[[7], [31]], phi:[[-6]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_9$, $ M_4$, $ M_8$, $ M_1$, $ M_7$, $ M_2$, $ M_3$, $ \phi_1q_2^2$, $ q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_9^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_4M_9$, $ M_8M_9$, $ M_1M_9$, $ M_7M_9$, $ M_4^2$, $ M_4M_8$, $ M_8^2$, $ \phi_1q_1q_2$, $ M_1M_4$, $ M_4M_7$, $ M_1M_8$, $ M_7M_8$, $ \phi_1q_1\tilde{q}_1$, $ M_1^2$, $ M_1M_7$, $ M_7^2$, $ M_2M_9$, $ \phi_1q_1\tilde{q}_2$, $ M_3M_9$, $ M_2M_4$, $ M_2M_8$, $ M_3M_4$, $ M_3M_8$, $ M_1M_2$, $ M_2M_7$, $ M_1M_3$, $ M_3M_7$, $ M_9\phi_1q_2^2$, $ M_9q_1\tilde{q}_2$ | . | -3 | t^2.14 + 2*t^2.41 + 2*t^2.62 + t^3.1 + t^3.18 + t^3.66 + t^3.79 + 2*t^4.07 + 2*t^4.27 + t^4.48 + 2*t^4.55 + 2*t^4.76 + 3*t^4.83 + 4*t^5.03 + 4*t^5.24 + t^5.31 + 2*t^5.52 + t^5.59 + 2*t^5.72 + t^5.8 + t^5.93 - 3*t^6. + 2*t^6.07 + 2*t^6.2 + 2*t^6.28 + t^6.35 + 3*t^6.41 + 2*t^6.48 + t^6.61 + 6*t^6.69 - t^6.76 + t^6.83 + 6*t^6.89 + 2*t^6.97 - t^7.04 + 2*t^7.1 + 3*t^7.17 + 3*t^7.24 + t^7.32 + 4*t^7.38 + 5*t^7.45 + t^7.58 + 5*t^7.65 + 2*t^7.73 + 5*t^7.86 + 3*t^7.93 + t^8. + t^8.06 + 2*t^8.14 + t^8.27 + 5*t^8.34 - 5*t^8.41 + 4*t^8.49 + 5*t^8.55 - 5*t^8.62 + 3*t^8.69 + 2*t^8.75 + t^8.77 + 4*t^8.82 + 2*t^8.9 + t^8.96 + 2*t^8.97 - t^4.45/y - t^6.59/y - t^6.86/y - t^7.07/y + t^7.27/y + (2*t^7.55)/y - t^7.62/y + (2*t^7.76)/y + (2*t^7.83)/y + (5*t^8.03)/y + (2*t^8.24)/y + (2*t^8.31)/y + (2*t^8.52)/y + (2*t^8.59)/y + t^8.72/y + (3*t^8.8)/y + t^8.93/y - t^4.45*y - t^6.59*y - t^6.86*y - t^7.07*y + t^7.27*y + 2*t^7.55*y - t^7.62*y + 2*t^7.76*y + 2*t^7.83*y + 5*t^8.03*y + 2*t^8.24*y + 2*t^8.31*y + 2*t^8.52*y + 2*t^8.59*y + t^8.72*y + 3*t^8.8*y + t^8.93*y | g1^16*t^2.14 + (2*t^2.41)/g1^10 + 2*g1^14*t^2.62 + g1^12*t^3.1 + t^3.18/g1^38 + t^3.66/g1^40 + g1^34*t^3.79 + 2*g1^8*t^4.07 + 2*g1^32*t^4.27 + g1^56*t^4.48 + 2*g1^6*t^4.55 + 2*g1^30*t^4.76 + (3*t^4.83)/g1^20 + 4*g1^4*t^5.03 + 4*g1^28*t^5.24 + t^5.31/g1^22 + 2*g1^2*t^5.52 + t^5.59/g1^48 + 2*g1^26*t^5.72 + t^5.8/g1^24 + g1^50*t^5.93 - 3*t^6. + (2*t^6.07)/g1^50 + 2*g1^24*t^6.2 + (2*t^6.28)/g1^26 + t^6.35/g1^76 + 3*g1^48*t^6.41 + (2*t^6.48)/g1^2 + g1^72*t^6.61 + 6*g1^22*t^6.69 - t^6.76/g1^28 + t^6.83/g1^78 + 6*g1^46*t^6.89 + (2*t^6.97)/g1^4 - t^7.04/g1^54 + 2*g1^70*t^7.1 + 3*g1^20*t^7.17 + (3*t^7.24)/g1^30 + t^7.32/g1^80 + 4*g1^44*t^7.38 + (5*t^7.45)/g1^6 + g1^68*t^7.58 + 5*g1^18*t^7.65 + (2*t^7.73)/g1^32 + 5*g1^42*t^7.86 + (3*t^7.93)/g1^8 + t^8./g1^58 + g1^66*t^8.06 + 2*g1^16*t^8.14 + g1^90*t^8.27 + 5*g1^40*t^8.34 - (5*t^8.41)/g1^10 + (4*t^8.49)/g1^60 + 5*g1^64*t^8.55 - 5*g1^14*t^8.62 + (3*t^8.69)/g1^36 + 2*g1^88*t^8.75 + t^8.77/g1^86 + 4*g1^38*t^8.82 + (2*t^8.9)/g1^12 + g1^112*t^8.96 + (2*t^8.97)/g1^62 - t^4.45/(g1^6*y) - (g1^10*t^6.59)/y - t^6.86/(g1^16*y) - (g1^8*t^7.07)/y + (g1^32*t^7.27)/y + (2*g1^6*t^7.55)/y - t^7.62/(g1^44*y) + (2*g1^30*t^7.76)/y + (2*t^7.83)/(g1^20*y) + (5*g1^4*t^8.03)/y + (2*g1^28*t^8.24)/y + (2*t^8.31)/(g1^22*y) + (2*g1^2*t^8.52)/y + (2*t^8.59)/(g1^48*y) + (g1^26*t^8.72)/y + (3*t^8.8)/(g1^24*y) + (g1^50*t^8.93)/y - (t^4.45*y)/g1^6 - g1^10*t^6.59*y - (t^6.86*y)/g1^16 - g1^8*t^7.07*y + g1^32*t^7.27*y + 2*g1^6*t^7.55*y - (t^7.62*y)/g1^44 + 2*g1^30*t^7.76*y + (2*t^7.83*y)/g1^20 + 5*g1^4*t^8.03*y + 2*g1^28*t^8.24*y + (2*t^8.31*y)/g1^22 + 2*g1^2*t^8.52*y + (2*t^8.59*y)/g1^48 + g1^26*t^8.72*y + (3*t^8.8*y)/g1^24 + g1^50*t^8.93*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 |
---|---|---|---|---|---|---|---|---|---|
4380 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_1$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_2\tilde{q}_1$ + $ M_4M_6$ + $ M_1M_5$ + $ M_5M_7$ + $ \phi_1q_1^2$ + $ M_6M_8$ | 0.6538 | 0.819 | 0.7983 | [X:[], M:[0.8755, 1.0361, 1.0523, 0.8032, 1.1245, 1.1968, 0.8755, 0.8032], q:[0.759, 0.3655], qb:[0.4377, 0.5099], phi:[0.4819]] | 2*t^2.41 + 2*t^2.63 + t^3.11 + t^3.16 + t^3.64 + t^3.81 + t^3.86 + 2*t^4.07 + t^4.29 + t^4.51 + 3*t^4.82 + 4*t^5.04 + 3*t^5.25 + 2*t^5.52 + t^5.57 + 2*t^5.73 - 3*t^6. - t^4.45/y - t^4.45*y | detail |