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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349 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1^2$ | 0.6617 | 0.8086 | 0.8182 | [X:[], M:[0.6944, 1.1019, 0.9956, 1.1019], q:[0.7755, 0.5301], qb:[0.4743, 0.4239], phi:[0.4491]] | [X:[], M:[[12, 12], [-4, -4], [7, 11], [-4, -4]], q:[[-1, -1], [-11, -11]], qb:[[4, 0], [0, 4]], phi:[[2, 2]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_1$, $ q_2\tilde{q}_2$, $ M_3$, $ M_2$, $ M_4$, $ q_1\tilde{q}_2$, $ q_1\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1^2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_2^2$, $ \phi_1q_1\tilde{q}_2$, $ M_1M_3$, $ M_1M_2$, $ M_1M_4$, $ q_2^2\tilde{q}_2^2$, $ M_3^2$, $ M_1\phi_1\tilde{q}_2^2$ | . | -3 | t^2.08 + t^2.86 + t^2.99 + 2*t^3.31 + t^3.6 + t^3.75 + t^3.89 + t^4.04 + t^4.17 + t^4.19 + t^4.21 + t^4.36 + t^4.53 + t^4.95 + t^5.07 + 2*t^5.39 + t^5.72 + 2*t^5.97 - 3*t^6. + t^6.12 - t^6.15 + t^6.17 + t^6.25 + t^6.28 + 2*t^6.29 - t^6.32 + t^6.46 + t^6.58 + 3*t^6.61 + t^6.75 + t^6.88 + t^6.9 + t^7.03 + t^7.05 + t^7.07 + t^7.15 + 2*t^7.2 + t^7.35 + t^7.39 + 2*t^7.47 + t^7.49 + t^7.5 + t^7.51 + t^7.64 + t^7.78 + t^7.79 + t^7.81 + t^7.83 + t^7.93 + t^7.94 + 2*t^8.06 - 2*t^8.08 + t^8.1 + t^8.21 + t^8.25 + t^8.33 + t^8.36 + 2*t^8.38 + t^8.39 - t^8.4 + t^8.42 + t^8.55 + t^8.59 + 2*t^8.69 + t^8.72 + t^8.74 + t^8.84 - 3*t^8.86 + t^8.89 + 2*t^8.96 - 3*t^8.99 - t^4.35/y - t^6.43/y + t^7.04/y - t^7.33/y + t^7.36/y - t^7.65/y + t^7.95/y + t^8.07/y + t^8.26/y + (2*t^8.39)/y - t^8.51/y + t^8.68/y + t^8.83/y + t^8.85/y + t^8.97/y - t^4.35*y - t^6.43*y + t^7.04*y - t^7.33*y + t^7.36*y - t^7.65*y + t^7.95*y + t^8.07*y + t^8.26*y + 2*t^8.39*y - t^8.51*y + t^8.68*y + t^8.83*y + t^8.85*y + t^8.97*y | g1^12*g2^12*t^2.08 + t^2.86/(g1^11*g2^7) + g1^7*g2^11*t^2.99 + (2*t^3.31)/(g1^4*g2^4) + (g2^3*t^3.6)/g1 + (g1^3*t^3.75)/g2 + g1^2*g2^10*t^3.89 + g1^6*g2^6*t^4.04 + g1^24*g2^24*t^4.17 + g1^10*g2^2*t^4.19 + t^4.21/(g1^9*g2^5) + t^4.36/(g1^5*g2^9) + t^4.53/(g1^20*g2^20) + g1*g2^5*t^4.95 + g1^19*g2^23*t^5.07 + 2*g1^8*g2^8*t^5.39 + t^5.72/(g1^22*g2^14) + 2*g1^14*g2^22*t^5.97 - 3*t^6. + g1^18*g2^18*t^6.12 - (g1^4*t^6.15)/g2^4 + t^6.17/(g1^15*g2^11) + g1^36*g2^36*t^6.25 + g1^22*g2^14*t^6.28 + 2*g1^3*g2^7*t^6.29 - t^6.32/(g1^11*g2^15) + t^6.46/(g1^12*g2^4) + g1^6*g2^14*t^6.58 + (3*t^6.61)/(g1^8*g2^8) + (g2^3*t^6.75)/g1^9 + g1^9*g2^21*t^6.88 + t^6.9/(g1^5*g2) + g1^13*g2^17*t^7.03 + t^7.05/(g1*g2^5) + t^7.07/(g1^20*g2^12) + g1^31*g2^35*t^7.15 + (2*g2^6*t^7.2)/g1^2 + g1^2*g2^2*t^7.35 + t^7.39/(g1^31*g2^27) + 2*g1^20*g2^20*t^7.47 + g1*g2^13*t^7.49 + (g1^6*t^7.5)/g2^2 + t^7.51/(g1^13*g2^9) + g1^5*g2^9*t^7.64 + g1^4*g2^20*t^7.78 + g1^9*g2^5*t^7.79 + t^7.81/(g1^10*g2^2) + t^7.83/(g1^24*g2^24) + g1^8*g2^16*t^7.93 + g1^13*g2*t^7.94 + 2*g1^26*g2^34*t^8.06 - 2*g1^12*g2^12*t^8.08 + (g2^5*t^8.1)/g1^7 + g1^30*g2^30*t^8.21 + (g2*t^8.25)/g1^3 + g1^48*g2^48*t^8.33 + g1^34*g2^26*t^8.36 + 2*g1^15*g2^19*t^8.38 + g1^20*g2^4*t^8.39 - (g1*t^8.4)/g2^3 + t^8.42/(g1^18*g2^10) + (g1^5*t^8.55)/g2^7 + t^8.59/(g1^33*g2^21) + 2*g1^4*g2^4*t^8.69 + t^8.72/(g1^10*g2^18) + t^8.74/(g1^29*g2^25) + g1^3*g2^15*t^8.84 - (3*t^8.86)/(g1^11*g2^7) + t^8.89/(g1^25*g2^29) + 2*g1^21*g2^33*t^8.96 - 3*g1^7*g2^11*t^8.99 - (g1^2*g2^2*t^4.35)/y - (g1^14*g2^14*t^6.43)/y + (g1^6*g2^6*t^7.04)/y - (g1^9*g2^13*t^7.33)/y + t^7.36/(g1^5*g2^9*y) - t^7.65/(g1^2*g2^2*y) + (g1*g2^5*t^7.95)/y + (g1^19*g2^23*t^8.07)/y + t^8.26/(g1^10*g2^10*y) + (2*g1^8*g2^8*t^8.39)/y - (g1^26*g2^26*t^8.51)/y + (g1^11*g2^15*t^8.68)/y + (g1^15*g2^11*t^8.83)/y + (g2^4*t^8.85)/(g1^4*y) + (g1^14*g2^22*t^8.97)/y - g1^2*g2^2*t^4.35*y - g1^14*g2^14*t^6.43*y + g1^6*g2^6*t^7.04*y - g1^9*g2^13*t^7.33*y + (t^7.36*y)/(g1^5*g2^9) - (t^7.65*y)/(g1^2*g2^2) + g1*g2^5*t^7.95*y + g1^19*g2^23*t^8.07*y + (t^8.26*y)/(g1^10*g2^10) + 2*g1^8*g2^8*t^8.39*y - g1^26*g2^26*t^8.51*y + g1^11*g2^15*t^8.68*y + g1^15*g2^11*t^8.83*y + (g2^4*t^8.85*y)/g1^4 + g1^14*g2^22*t^8.97*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 |
---|---|---|---|---|---|---|---|---|---|
219 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_1$ | 0.6711 | 0.825 | 0.8135 | [X:[], M:[0.6804, 1.1065, 0.9852], q:[0.7766, 0.543], qb:[0.4718, 0.4217], phi:[0.4467]] | t^2.04 + t^2.68 + t^2.89 + t^2.96 + t^3.32 + t^3.59 + t^3.75 + t^3.87 + t^4.02 + t^4.08 + t^4.17 + t^4.23 + t^4.38 + t^4.6 + t^4.72 + t^4.94 + t^5. + 2*t^5.36 + t^5.57 + t^5.64 + t^5.79 + 2*t^5.91 - 2*t^6. - t^4.34/y - t^4.34*y | detail |