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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46209 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_2\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4\phi_1^2$ + $ M_2^2$ | 0.5924 | 0.7275 | 0.8144 | [X:[], M:[0.7021, 1.0, 0.845, 1.2265], q:[0.3423, 0.9556], qb:[0.6577, 0.4974], phi:[0.3868]] | [X:[], M:[[7, -1], [0, 0], [-3, -3], [-2, 2]], q:[[-3, 0], [-4, 1]], qb:[[3, 0], [0, 3]], phi:[[1, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_1$, $ q_1\tilde{q}_2$, $ M_3$, $ M_2$, $ \phi_1q_1^2$, $ M_4$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_1^2$, $ q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1M_3$, $ q_2\tilde{q}_1$, $ q_1^2\tilde{q}_2^2$, $ \phi_1q_1q_2$, $ M_3q_1\tilde{q}_2$, $ M_3^2$, $ M_1M_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_1^3\tilde{q}_2$, $ M_3\phi_1q_1^2$, $ M_1M_4$ | . | -2 | t^2.11 + t^2.52 + t^2.53 + t^3. + t^3.21 + 2*t^3.68 + t^4.14 + t^4.21 + t^4.36 + t^4.63 + t^4.64 + t^4.84 + t^5.04 + t^5.05 + t^5.07 + t^5.11 + t^5.52 + t^5.73 + t^5.75 + t^5.79 - 2*t^6. + 2*t^6.2 + 2*t^6.21 + t^6.25 + t^6.32 + t^6.43 - t^6.48 + t^6.66 + t^6.68 - t^6.7 + t^6.73 + t^6.75 + t^6.88 + 2*t^6.89 + t^7.14 - t^7.16 + t^7.18 + t^7.21 + 3*t^7.36 + t^7.56 + t^7.57 + t^7.59 + t^7.6 + t^7.82 - t^7.84 + t^7.89 + 2*t^8.04 - 2*t^8.11 + t^8.25 + t^8.27 + t^8.28 + t^8.29 + t^8.32 + t^8.36 + t^8.43 + t^8.5 - 2*t^8.52 - 3*t^8.53 - t^8.59 + 3*t^8.72 + t^8.73 + t^8.75 + t^8.77 + t^8.84 + t^8.85 + t^8.95 + t^8.96 - t^4.16/y - t^6.27/y - t^6.7/y + (2*t^7.63)/y + t^7.64/y + (2*t^8.05)/y + t^8.11/y + t^8.32/y - t^8.37/y + t^8.52/y + t^8.53/y + t^8.73/y + t^8.75/y + (2*t^8.79)/y - t^8.8/y - t^4.16*y - t^6.27*y - t^6.7*y + 2*t^7.63*y + t^7.64*y + 2*t^8.05*y + t^8.11*y + t^8.32*y - t^8.37*y + t^8.52*y + t^8.53*y + t^8.73*y + t^8.75*y + 2*t^8.79*y - t^8.8*y | (g1^7*t^2.11)/g2 + (g2^3*t^2.52)/g1^3 + t^2.53/(g1^3*g2^3) + t^3. + t^3.21/(g1^5*g2) + (2*g2^2*t^3.68)/g1^2 + g1*g2^5*t^4.14 + (g1^14*t^4.21)/g2^2 + (g2^4*t^4.36)/g1^4 + g1^4*g2^2*t^4.63 + (g1^4*t^4.64)/g2^4 + (g2*t^4.84)/g1 + (g2^6*t^5.04)/g1^6 + t^5.05/g1^6 + t^5.07/(g1^6*g2^6) + (g1^7*t^5.11)/g2 + (g2^3*t^5.52)/g1^3 + (g2^2*t^5.73)/g1^8 + t^5.75/(g1^8*g2^4) + g1^5*g2*t^5.79 - 2*t^6. + (2*g2^5*t^6.2)/g1^5 + (2*t^6.21)/(g1^5*g2) + g1^8*g2^4*t^6.25 + (g1^21*t^6.32)/g2^3 + t^6.43/(g1^10*g2^2) - (g1^3*t^6.48)/g2^3 + (g2^8*t^6.66)/g1^2 + (g2^2*t^6.68)/g1^2 - t^6.7/(g1^2*g2^4) + g1^11*g2*t^6.73 + (g1^11*t^6.75)/g2^5 + (g2^7*t^6.88)/g1^7 + (2*g2*t^6.89)/g1^7 + g1*g2^5*t^7.14 - (g1*t^7.16)/g2 + (g1*t^7.18)/g2^7 + (g1^14*t^7.21)/g2^2 + (3*g2^4*t^7.36)/g1^4 + (g2^9*t^7.56)/g1^9 + (g2^3*t^7.57)/g1^9 + t^7.59/(g1^9*g2^3) + t^7.6/(g1^9*g2^9) + (g2^7*t^7.82)/g1 - (g2*t^7.84)/g1 + g1^12*t^7.89 + (2*g2^6*t^8.04)/g1^6 - (2*g1^7*t^8.11)/g2 + (g2^5*t^8.25)/g1^11 + t^8.27/(g1^11*g2) + t^8.28/(g1^11*g2^7) + g1^2*g2^10*t^8.29 + (g1^2*t^8.32)/g2^2 + g1^15*g2^3*t^8.36 + (g1^28*t^8.43)/g2^4 + (g2^9*t^8.5)/g1^3 - (2*g2^3*t^8.52)/g1^3 - (3*t^8.53)/(g1^3*g2^3) - (g1^10*t^8.59)/g2^4 + (3*g2^8*t^8.72)/g1^8 + (g2^2*t^8.73)/g1^8 + t^8.75/(g1^8*g2^4) + g1^5*g2^7*t^8.77 + g1^18*t^8.84 + (g1^18*t^8.85)/g2^6 + (g2*t^8.95)/g1^13 + t^8.96/(g1^13*g2^5) - (g1*t^4.16)/(g2*y) - (g1^8*t^6.27)/(g2^2*y) - t^6.7/(g1^2*g2^4*y) + (2*g1^4*g2^2*t^7.63)/y + (g1^4*t^7.64)/(g2^4*y) + (2*t^8.05)/(g1^6*y) + (g1^7*t^8.11)/(g2*y) + (g1^2*t^8.32)/(g2^2*y) - (g1^15*t^8.37)/(g2^3*y) + (g2^3*t^8.52)/(g1^3*y) + t^8.53/(g1^3*g2^3*y) + (g2^2*t^8.73)/(g1^8*y) + t^8.75/(g1^8*g2^4*y) + (2*g1^5*g2*t^8.79)/y - (g1^5*t^8.8)/(g2^5*y) - (g1*t^4.16*y)/g2 - (g1^8*t^6.27*y)/g2^2 - (t^6.7*y)/(g1^2*g2^4) + 2*g1^4*g2^2*t^7.63*y + (g1^4*t^7.64*y)/g2^4 + (2*t^8.05*y)/g1^6 + (g1^7*t^8.11*y)/g2 + (g1^2*t^8.32*y)/g2^2 - (g1^15*t^8.37*y)/g2^3 + (g2^3*t^8.52*y)/g1^3 + (t^8.53*y)/(g1^3*g2^3) + (g2^2*t^8.73*y)/g1^8 + (t^8.75*y)/(g1^8*g2^4) + 2*g1^5*g2*t^8.79*y - (g1^5*t^8.8*y)/g2^5 |
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 |
---|---|---|---|---|---|---|---|---|---|
45939 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_2\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4\phi_1^2$ | 0.6485 | 0.7963 | 0.8144 | [X:[], M:[0.7078, 0.6913, 0.7007, 1.2958], q:[0.4766, 0.8157], qb:[0.8322, 0.4671], phi:[0.3521]] | t^2.07 + t^2.1 + t^2.12 + t^2.83 + t^3.85 + t^3.86 + 2*t^3.89 + t^3.92 + t^4.15 + t^4.18 + 2*t^4.2 + t^4.23 + t^4.25 + t^4.9 + t^4.93 + t^4.94 + t^4.95 + t^5.66 + t^5.92 + t^5.93 + t^5.95 + 2*t^5.96 + t^5.98 + 2*t^5.99 - 3*t^6. - t^4.06/y - t^4.06*y | detail |