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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57137 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1\phi_1^2$ + $ \phi_1\tilde{q}_1^2$ + $ M_3M_4$ + $ M_5\phi_1^2$ + $ M_6\phi_1q_2\tilde{q}_2$ + $ M_7\phi_1\tilde{q}_2^2$ | 0.6957 | 0.8901 | 0.7816 | [X:[], M:[1.0548, 0.7259, 0.8356, 1.1644, 1.0548, 0.6918, 0.7259], q:[0.5103, 0.4348], qb:[0.7637, 0.4007], phi:[0.4726]] | [X:[], M:[[4], [-20], [-12], [12], [4], [14], [-20]], q:[[19], [-23]], qb:[[1], [11]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_6$, $ M_2$, $ M_7$, $ M_3$, $ q_1\tilde{q}_2$, $ M_1$, $ M_5$, $ M_4$, $ q_2\tilde{q}_1$, $ \phi_1q_2^2$, $ M_6^2$, $ \phi_1q_1\tilde{q}_2$, $ M_2M_6$, $ M_6M_7$, $ \phi_1q_1q_2$, $ M_2^2$, $ M_2M_7$, $ M_7^2$, $ \phi_1q_1^2$, $ M_3M_6$, $ M_2M_3$, $ M_3M_7$, $ M_6q_1\tilde{q}_2$, $ M_7q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_3^2$, $ \phi_1q_2\tilde{q}_1$, $ M_1M_6$, $ M_5M_6$, $ \phi_1q_1\tilde{q}_1$, $ M_3q_1\tilde{q}_2$, $ M_1M_2$, $ M_2M_5$, $ M_1M_7$, $ M_5M_7$, $ q_1^2\tilde{q}_2^2$, $ M_4M_6$, $ M_1M_3$, $ M_2M_4$, $ M_3M_5$, $ M_4M_7$, $ M_6q_2\tilde{q}_1$, $ M_2q_2\tilde{q}_1$, $ M_7q_2\tilde{q}_1$, $ M_5q_1\tilde{q}_2$ | . | -2 | t^2.08 + 2*t^2.18 + t^2.51 + t^2.73 + 2*t^3.16 + t^3.49 + t^3.6 + t^4.03 + 2*t^4.15 + 3*t^4.25 + 3*t^4.36 + t^4.48 + t^4.58 + 2*t^4.68 + t^4.81 + 2*t^4.91 + t^5.01 + 3*t^5.24 + 4*t^5.34 + t^5.47 + t^5.57 + 4*t^5.67 + t^5.77 + t^5.9 - 2*t^6. + t^6.1 + 2*t^6.2 + 2*t^6.23 + 6*t^6.33 + 4*t^6.43 + 5*t^6.53 + t^6.56 + 4*t^6.66 + 4*t^6.76 + 3*t^6.86 + 2*t^6.88 + 2*t^6.99 + 2*t^7.09 + 3*t^7.19 + t^7.21 + 3*t^7.32 + 4*t^7.42 + 6*t^7.52 + t^7.54 + t^7.62 + 3*t^7.64 + 4*t^7.75 + 5*t^7.85 + t^7.95 + 2*t^7.97 + t^8.05 - 2*t^8.08 - 3*t^8.18 + t^8.2 + 2*t^8.28 + 2*t^8.3 + 3*t^8.38 + 5*t^8.4 + 7*t^8.51 + 6*t^8.61 + 3*t^8.63 + 7*t^8.71 + 2*t^8.73 + 7*t^8.84 + 5*t^8.94 + 3*t^8.96 - t^4.42/y - t^6.49/y - (2*t^6.6)/y + (3*t^7.25)/y + t^7.36/y + (2*t^7.68)/y + t^7.81/y + (2*t^7.91)/y + (5*t^8.24)/y + (5*t^8.34)/y + (3*t^8.67)/y - t^8.77/y + (2*t^8.9)/y - t^4.42*y - t^6.49*y - 2*t^6.6*y + 3*t^7.25*y + t^7.36*y + 2*t^7.68*y + t^7.81*y + 2*t^7.91*y + 5*t^8.24*y + 5*t^8.34*y + 3*t^8.67*y - t^8.77*y + 2*t^8.9*y | g1^14*t^2.08 + (2*t^2.18)/g1^20 + t^2.51/g1^12 + g1^30*t^2.73 + 2*g1^4*t^3.16 + g1^12*t^3.49 + t^3.6/g1^22 + t^4.03/g1^48 + 2*g1^28*t^4.15 + (3*t^4.25)/g1^6 + (3*t^4.36)/g1^40 + g1^36*t^4.48 + g1^2*t^4.58 + (2*t^4.68)/g1^32 + g1^44*t^4.81 + 2*g1^10*t^4.91 + t^5.01/g1^24 + 3*g1^18*t^5.24 + (4*t^5.34)/g1^16 + g1^60*t^5.47 + g1^26*t^5.57 + (4*t^5.67)/g1^8 + t^5.77/g1^42 + g1^34*t^5.9 - 2*t^6. + t^6.1/g1^34 + (2*t^6.2)/g1^68 + 2*g1^42*t^6.23 + 6*g1^8*t^6.33 + (4*t^6.43)/g1^26 + (5*t^6.53)/g1^60 + g1^50*t^6.56 + 4*g1^16*t^6.66 + (4*t^6.76)/g1^18 + (3*t^6.86)/g1^52 + 2*g1^58*t^6.88 + 2*g1^24*t^6.99 + (2*t^7.09)/g1^10 + (3*t^7.19)/g1^44 + g1^66*t^7.21 + 3*g1^32*t^7.32 + (4*t^7.42)/g1^2 + (6*t^7.52)/g1^36 + g1^74*t^7.54 + t^7.62/g1^70 + 3*g1^40*t^7.64 + 4*g1^6*t^7.75 + (5*t^7.85)/g1^28 + t^7.95/g1^62 + 2*g1^48*t^7.97 + t^8.05/g1^96 - 2*g1^14*t^8.08 - (3*t^8.18)/g1^20 + g1^90*t^8.2 + (2*t^8.28)/g1^54 + 2*g1^56*t^8.3 + (3*t^8.38)/g1^88 + 5*g1^22*t^8.4 + (7*t^8.51)/g1^12 + (6*t^8.61)/g1^46 + 3*g1^64*t^8.63 + (7*t^8.71)/g1^80 + 2*g1^30*t^8.73 + (7*t^8.84)/g1^4 + (5*t^8.94)/g1^38 + 3*g1^72*t^8.96 - t^4.42/(g1^2*y) - (g1^12*t^6.49)/y - (2*t^6.6)/(g1^22*y) + (3*t^7.25)/(g1^6*y) + t^7.36/(g1^40*y) + (2*t^7.68)/(g1^32*y) + (g1^44*t^7.81)/y + (2*g1^10*t^7.91)/y + (5*g1^18*t^8.24)/y + (5*t^8.34)/(g1^16*y) + (3*t^8.67)/(g1^8*y) - t^8.77/(g1^42*y) + (2*g1^34*t^8.9)/y - (t^4.42*y)/g1^2 - g1^12*t^6.49*y - (2*t^6.6*y)/g1^22 + (3*t^7.25*y)/g1^6 + (t^7.36*y)/g1^40 + (2*t^7.68*y)/g1^32 + g1^44*t^7.81*y + 2*g1^10*t^7.91*y + 5*g1^18*t^8.24*y + (5*t^8.34*y)/g1^16 + (3*t^8.67*y)/g1^8 - (t^8.77*y)/g1^42 + 2*g1^34*t^8.9*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 |
---|---|---|---|---|---|---|---|---|---|
55563 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1\phi_1^2$ + $ \phi_1\tilde{q}_1^2$ + $ M_3M_4$ + $ M_5\phi_1^2$ + $ M_6\phi_1q_2\tilde{q}_2$ | 0.6759 | 0.8533 | 0.7921 | [X:[], M:[1.0537, 0.7316, 0.839, 1.161, 1.0537, 0.6879], q:[0.505, 0.4414], qb:[0.7634, 0.3976], phi:[0.4732]] | t^2.06 + t^2.19 + t^2.52 + t^2.71 + 2*t^3.16 + t^3.48 + t^3.61 + t^3.81 + t^4.07 + 2*t^4.13 + 2*t^4.26 + t^4.39 + t^4.45 + t^4.58 + t^4.71 + t^4.77 + t^4.9 + t^5.03 + 3*t^5.22 + 2*t^5.36 + t^5.42 + t^5.55 + 3*t^5.68 + 2*t^5.87 - t^6. - t^4.42/y - t^4.42*y | detail |