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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1911 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_3\phi_1q_2\tilde{q}_1$ + $ M_2M_3$ + $ M_4\phi_1q_2\tilde{q}_2$ + $ M_5q_1\tilde{q}_2$ | 0.6223 | 0.8259 | 0.7535 | [X:[], M:[0.9307, 1.208, 0.792, 0.6733, 0.812], q:[0.7327, 0.3367], qb:[0.3367, 0.4554], phi:[0.5347]] | [X:[], M:[[4], [-12], [12], [-10], [-18]], q:[[1], [-5]], qb:[[-5], [17]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_4$, $ q_2\tilde{q}_1$, $ M_3$, $ q_2\tilde{q}_2$, $ M_5$, $ M_1$, $ \phi_1^2$, $ q_1\tilde{q}_1$, $ M_2$, $ \phi_1q_2^2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_4^2$, $ M_4q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ \phi_1\tilde{q}_2^2$, $ M_3M_4$, $ M_3q_2\tilde{q}_1$, $ M_4q_2\tilde{q}_2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ M_4M_5$, $ M_5q_2\tilde{q}_1$, $ M_3^2$, $ M_3q_2\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_1M_4$, $ M_3M_5$, $ \phi_1q_1q_2$, $ \phi_1q_1\tilde{q}_1$, $ M_5q_2\tilde{q}_2$, $ M_5^2$, $ M_1M_3$, $ \phi_1q_1\tilde{q}_2$, $ M_1M_5$, $ M_4\phi_1^2$, $ M_4q_1\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ q_1q_2\tilde{q}_1^2$, $ M_1^2$, $ M_3\phi_1^2$, $ M_3q_1\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_2$, $ M_2M_4$, $ M_5\phi_1^2$, $ M_4\phi_1q_2^2$, $ M_5q_1\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_1$, $ M_4\phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_1^3$ | $M_3\phi_1q_2^2$, $ M_3\phi_1\tilde{q}_1^2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_4\phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1^2\tilde{q}_2$ | 3 | 2*t^2.02 + 2*t^2.38 + t^2.44 + t^2.79 + 2*t^3.21 + 3*t^3.62 + t^3.98 + 3*t^4.04 + t^4.34 + 4*t^4.4 + 2*t^4.46 + 3*t^4.75 + 4*t^4.81 + t^4.87 + 2*t^5.17 + 5*t^5.23 + 4*t^5.58 + 6*t^5.64 + 3*t^6. + 7*t^6.06 + t^6.36 + 8*t^6.42 + 3*t^6.48 + 2*t^6.71 + 5*t^6.77 + 10*t^6.83 + 2*t^6.89 + 4*t^7.13 + 3*t^7.19 + 13*t^7.25 + t^7.31 + 3*t^7.54 + 5*t^7.6 + 10*t^7.66 + 4*t^7.96 + 5*t^8.02 + 11*t^8.08 + t^8.32 + 11*t^8.44 + 7*t^8.5 + t^8.67 + t^8.73 + 3*t^8.79 + 15*t^8.85 + 3*t^8.91 - t^4.6/y - t^6.62/y + (4*t^7.4)/y + (2*t^7.46)/y + t^7.75/y + (4*t^7.81)/y + (3*t^8.17)/y + (5*t^8.23)/y + (5*t^8.58)/y + (7*t^8.64)/y - t^4.6*y - t^6.62*y + 4*t^7.4*y + 2*t^7.46*y + t^7.75*y + 4*t^7.81*y + 3*t^8.17*y + 5*t^8.23*y + 5*t^8.58*y + 7*t^8.64*y | (2*t^2.02)/g1^10 + 2*g1^12*t^2.38 + t^2.44/g1^18 + g1^4*t^2.79 + (2*t^3.21)/g1^4 + (3*t^3.62)/g1^12 + g1^10*t^3.98 + (3*t^4.04)/g1^20 + g1^32*t^4.34 + 4*g1^2*t^4.4 + (2*t^4.46)/g1^28 + 3*g1^24*t^4.75 + (4*t^4.81)/g1^6 + t^4.87/g1^36 + 2*g1^16*t^5.17 + (5*t^5.23)/g1^14 + 4*g1^8*t^5.58 + (6*t^5.64)/g1^22 + 3*t^6. + (7*t^6.06)/g1^30 + g1^22*t^6.36 + (8*t^6.42)/g1^8 + (3*t^6.48)/g1^38 + 2*g1^44*t^6.71 + 5*g1^14*t^6.77 + (10*t^6.83)/g1^16 + (2*t^6.89)/g1^46 + 4*g1^36*t^7.13 + 3*g1^6*t^7.19 + (13*t^7.25)/g1^24 + t^7.31/g1^54 + 3*g1^28*t^7.54 + (5*t^7.6)/g1^2 + (10*t^7.66)/g1^32 + 4*g1^20*t^7.96 + (5*t^8.02)/g1^10 + (11*t^8.08)/g1^40 + g1^42*t^8.32 + (11*t^8.44)/g1^18 + (7*t^8.5)/g1^48 + g1^64*t^8.67 + g1^34*t^8.73 + 3*g1^4*t^8.79 + (15*t^8.85)/g1^26 + (3*t^8.91)/g1^56 - t^4.6/(g1^2*y) - t^6.62/(g1^12*y) + (4*g1^2*t^7.4)/y + (2*t^7.46)/(g1^28*y) + (g1^24*t^7.75)/y + (4*t^7.81)/(g1^6*y) + (3*g1^16*t^8.17)/y + (5*t^8.23)/(g1^14*y) + (5*g1^8*t^8.58)/y + (7*t^8.64)/(g1^22*y) - (t^4.6*y)/g1^2 - (t^6.62*y)/g1^12 + 4*g1^2*t^7.4*y + (2*t^7.46*y)/g1^28 + g1^24*t^7.75*y + (4*t^7.81*y)/g1^6 + 3*g1^16*t^8.17*y + (5*t^8.23*y)/g1^14 + 5*g1^8*t^8.58*y + (7*t^8.64*y)/g1^22 |
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 |
---|---|---|---|---|---|---|---|---|---|
565 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_3\phi_1q_2\tilde{q}_1$ + $ M_2M_3$ + $ M_4\phi_1q_2\tilde{q}_2$ | 0.6075 | 0.7997 | 0.7596 | [X:[], M:[0.9243, 1.2271, 0.7729, 0.6893], q:[0.7311, 0.3446], qb:[0.3446, 0.4283], phi:[0.5379]] | 2*t^2.07 + 2*t^2.32 + t^2.77 + 2*t^3.23 + t^3.48 + 3*t^3.68 + t^3.93 + 3*t^4.14 + t^4.18 + 4*t^4.39 + 3*t^4.64 + 2*t^4.84 + 2*t^5.09 + 4*t^5.29 + 6*t^5.55 + 4*t^5.75 + 2*t^5.8 + 3*t^6. - t^4.61/y - t^4.61*y | detail |