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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57895 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ | 1.4146 | 1.6232 | 0.8715 | [X:[], M:[0.8781, 1.2975], q:[0.4137, 0.5212], qb:[0.3569, 0.6006], phi:[0.3513]] | [X:[], M:[[5, -5], [-4, 4]], q:[[-17, 7], [-5, -5]], qb:[[10, 0], [0, 10]], phi:[[2, -2]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$ | ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}^{2}$ | -1 | t^2.31 + 2*t^2.63 + t^3.04 + t^3.16 + t^3.37 + t^3.69 + t^3.89 + t^4.1 + 2*t^4.42 + t^4.62 + t^4.74 + 2*t^4.95 + t^5. + t^5.1 + t^5.15 + 2*t^5.27 + t^5.35 + t^5.42 + 2*t^5.47 + 2*t^5.68 + t^5.73 + 2*t^5.8 - t^6. + t^6.05 + t^6.09 + t^6.15 + 2*t^6.2 + t^6.32 + t^6.37 + 2*t^6.41 + t^6.48 + 3*t^6.53 + 4*t^6.73 + t^6.78 + t^6.85 + t^6.88 + 2*t^6.94 - t^7. + 4*t^7.05 + t^7.1 + t^7.14 + t^7.21 + 3*t^7.26 + t^7.38 + t^7.41 + 4*t^7.46 + t^7.53 + 4*t^7.58 + t^7.67 + t^7.73 + 6*t^7.78 + t^7.84 + t^7.85 + 3*t^7.9 - t^7.95 + 2*t^7.99 + 2*t^8.04 + 5*t^8.11 + t^8.14 + t^8.16 + 2*t^8.19 + t^8.26 + 2*t^8.36 - t^8.38 + t^8.4 + 2*t^8.43 + 2*t^8.47 + 6*t^8.52 + t^8.57 + t^8.58 - 3*t^8.63 + t^8.69 + 3*t^8.72 + t^8.77 + t^8.79 + 8*t^8.84 + t^8.89 + t^8.96 - t^4.05/y - t^5.11/y - t^6.37/y - (2*t^6.69)/y - t^7.1/y - t^7.22/y - t^7.42/y - (2*t^7.74)/y + (2*t^7.95)/y - t^8.15/y + t^8.35/y + (2*t^8.68)/y + t^8.8/y - t^4.05*y - t^5.11*y - t^6.37*y - 2*t^6.69*y - t^7.1*y - t^7.22*y - t^7.42*y - 2*t^7.74*y + 2*t^7.95*y - t^8.15*y + t^8.35*y + 2*t^8.68*y + t^8.8*y | (g2^7*t^2.31)/g1^7 + (2*g1^5*t^2.63)/g2^5 + (g2^17*t^3.04)/g1^17 + (g1^6*t^3.16)/g2^6 + (g2^5*t^3.37)/g1^5 + (g1^7*t^3.69)/g2^7 + (g2^4*t^3.89)/g1^4 + (g2^15*t^4.1)/g1^15 + (2*g2^3*t^4.42)/g1^3 + (g2^14*t^4.62)/g1^14 + (g1^9*t^4.74)/g2^9 + (2*g2^2*t^4.95)/g1^2 + g1^22*g2^8*t^5. + (g2^7*t^5.1)/g1^37 + (g2^13*t^5.15)/g1^13 + (2*g1^10*t^5.27)/g2^10 + (g2^24*t^5.35)/g1^24 + t^5.42/(g1^25*g2^5) + (2*g2*t^5.47)/g1 + (2*g2^12*t^5.68)/g1^12 + g1^12*g2^18*t^5.73 + (2*g1^11*t^5.8)/g2^11 - t^6. + g1^24*g2^6*t^6.05 + (g2^34*t^6.09)/g1^34 + (g2^5*t^6.15)/g1^35 + (2*g2^11*t^6.2)/g1^11 + (g1^12*t^6.32)/g2^12 + (g1^36*t^6.37)/g2^6 + (2*g2^22*t^6.41)/g1^22 + t^6.48/(g1^23*g2^7) + (3*g1*t^6.53)/g2 + (4*g2^10*t^6.73)/g1^10 + g1^14*g2^16*t^6.78 + (g1^13*t^6.85)/g2^13 + (g2^15*t^6.88)/g1^45 + (2*g2^21*t^6.94)/g1^21 - t^7./(g1^22*g2^8) + (4*g1^2*t^7.05)/g2^2 + g1^26*g2^4*t^7.1 + (g2^32*t^7.14)/g1^32 + (g2^3*t^7.21)/g1^33 + (3*g2^9*t^7.26)/g1^9 + (g1^14*t^7.38)/g2^14 + (g2^14*t^7.41)/g1^44 + (4*g2^20*t^7.46)/g1^20 + t^7.53/(g1^21*g2^9) + (4*g1^3*t^7.58)/g2^3 + (g2^31*t^7.67)/g1^31 + (g2^2*t^7.73)/g1^32 + (6*g2^8*t^7.78)/g1^8 + g1^16*g2^14*t^7.84 + t^7.85/(g1^9*g2^21) + (3*g1^15*t^7.9)/g2^15 - (g1^39*t^7.95)/g2^9 + (2*g2^19*t^7.99)/g1^19 + 2*g1^5*g2^25*t^8.04 + (5*g1^4*t^8.11)/g2^4 + (g2^24*t^8.14)/g1^54 + g1^28*g2^2*t^8.16 + (2*g2^30*t^8.19)/g1^30 + (g2*t^8.26)/g1^31 + 2*g1^17*g2^13*t^8.36 - t^8.38/(g1^8*g2^22) + (g2^41*t^8.4)/g1^41 + (2*g1^16*t^8.43)/g2^16 + (2*g2^12*t^8.47)/g1^42 + (6*g2^18*t^8.52)/g1^18 + g1^6*g2^24*t^8.57 + t^8.58/(g1^19*g2^11) - (3*g1^5*t^8.63)/g2^5 + g1^29*g2*t^8.69 + (3*g2^29*t^8.72)/g1^29 + (g2^35*t^8.77)/g1^5 + t^8.79/g1^30 + (8*g2^6*t^8.84)/g1^6 + g1^18*g2^12*t^8.89 + (g1^17*t^8.96)/g2^17 - (g1^2*t^4.05)/(g2^2*y) - (g1^4*t^5.11)/(g2^4*y) - (g2^5*t^6.37)/(g1^5*y) - (2*g1^7*t^6.69)/(g2^7*y) - (g2^15*t^7.1)/(g1^15*y) - (g1^8*t^7.22)/(g2^8*y) - (g2^3*t^7.42)/(g1^3*y) - (2*g1^9*t^7.74)/(g2^9*y) + (2*g2^2*t^7.95)/(g1^2*y) - (g2^13*t^8.15)/(g1^13*y) + (g2^24*t^8.35)/(g1^24*y) + (2*g2^12*t^8.68)/(g1^12*y) + (g1^11*t^8.8)/(g2^11*y) - (g1^2*t^4.05*y)/g2^2 - (g1^4*t^5.11*y)/g2^4 - (g2^5*t^6.37*y)/g1^5 - (2*g1^7*t^6.69*y)/g2^7 - (g2^15*t^7.1*y)/g1^15 - (g1^8*t^7.22*y)/g2^8 - (g2^3*t^7.42*y)/g1^3 - (2*g1^9*t^7.74*y)/g2^9 + (2*g2^2*t^7.95*y)/g1^2 - (g2^13*t^8.15*y)/g1^13 + (g2^24*t^8.35*y)/g1^24 + (2*g2^12*t^8.68*y)/g1^12 + (g1^11*t^8.8*y)/g2^11 |
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 |
---|---|---|---|---|---|---|---|---|---|
57292 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | 1.4741 | 1.6832 | 0.8758 | [M:[0.6739, 1.3301], q:[0.4928, 0.5024], qb:[0.4984, 0.4968], phi:[0.3349]] | t^2.022 + t^2.969 + t^2.974 + t^2.998 + t^3.002 + t^3.014 + t^3.974 + t^3.99 + t^4.002 + t^4.007 + t^4.043 + t^4.978 + t^4.983 + t^4.99 + t^4.995 + t^5.007 + t^5.012 + t^5.019 + t^5.024 + t^5.036 + t^5.469 + t^5.481 + t^5.485 + t^5.498 + t^5.938 + t^5.942 + t^5.947 + t^5.967 + t^5.971 + t^5.976 + t^5.983 + t^5.988 + t^5.995 - 3*t^6. - t^4.005/y - t^5.01/y - t^4.005*y - t^5.01*y | detail |