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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57950 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ | 1.4238 | 1.6034 | 0.888 | [X:[1.3758], M:[0.7803, 1.0924], q:[0.4516, 0.6038], qb:[0.456, 0.616], phi:[0.3121]] | [X:[[0, 4]], M:[[0, -5], [0, -7]], q:[[2, 5], [-1, 5]], qb:[[-2, 2], [1, 0]], phi:[[0, -2]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$ | ${}$ | -2 | t^2.34 + t^2.81 + t^3.18 + t^3.2 + t^3.28 + t^3.66 + t^4.12 + t^4.13 + t^4.14 + 2*t^4.6 + t^4.68 + t^5.05 + t^5.08 + t^5.15 + t^5.46 + t^5.52 + t^5.53 + 2*t^5.62 + t^5.91 + t^5.99 - 2*t^6. + t^6.01 + t^6.09 + t^6.36 + t^6.38 + t^6.39 + t^6.41 + t^6.46 + 2*t^6.47 + t^6.55 + t^6.84 + t^6.85 + t^6.86 + t^6.87 + t^6.91 + t^6.92 + 2*t^6.94 + t^6.95 + t^7.02 + t^7.29 + t^7.31 + 2*t^7.32 + 2*t^7.33 + t^7.34 + t^7.39 + 2*t^7.4 + t^7.49 + 3*t^7.77 + t^7.79 + 2*t^7.8 + 2*t^7.87 + t^7.88 + 2*t^7.96 + 2*t^8.23 + t^8.24 + 4*t^8.25 + t^8.27 + t^8.28 - t^8.32 + t^8.33 - 2*t^8.34 + t^8.35 + 2*t^8.43 + t^8.64 + t^8.66 + t^8.7 + 3*t^8.71 + t^8.72 + 3*t^8.73 + t^8.81 + 2*t^8.89 + t^8.81/y^2 - t^3.94/y - t^4.87/y - t^6.28/y - t^6.75/y - t^7.12/y - t^7.14/y - (2*t^7.21)/y - t^7.68/y - t^8.05/y - t^8.08/y + t^8.52/y - t^8.53/y + t^8.54/y - t^3.94*y - t^4.87*y - t^6.28*y - t^6.75*y - t^7.12*y - t^7.14*y - 2*t^7.21*y - t^7.68*y - t^8.05*y - t^8.08*y + t^8.52*y - t^8.53*y + t^8.54*y + t^8.81*y^2 | t^2.34/g2^5 + t^2.81/g2^6 + (g2^7*t^3.18)/g1^3 + g1^3*g2^5*t^3.2 + t^3.28/g2^7 + g2^5*t^3.66 + (g2^5*t^4.12)/g1^3 + g2^4*t^4.13 + g1^3*g2^3*t^4.14 + 2*g2^3*t^4.6 + t^4.68/g2^10 + (g2^3*t^5.05)/g1^3 + g1^3*g2*t^5.08 + t^5.15/g2^11 + g1^3*g2^13*t^5.46 + (g2^2*t^5.52)/g1^3 + g2*t^5.53 + (2*t^5.62)/g2^12 + g2^13*t^5.91 + (g2*t^5.99)/g1^3 - 2*t^6. + (g1^3*t^6.01)/g2 + t^6.09/g2^13 + (g2^14*t^6.36)/g1^6 + g2^12*t^6.38 + g1^3*g2^11*t^6.39 + g1^6*g2^10*t^6.41 + t^6.46/g1^3 + (2*t^6.47)/g2 + t^6.55/g2^14 + (g2^12*t^6.84)/g1^3 + g2^11*t^6.85 + g1^3*g2^10*t^6.86 + g1^6*g2^9*t^6.87 + t^6.91/g1^6 + t^6.92/(g1^3*g2) + (2*t^6.94)/g2^2 + (g1^3*t^6.95)/g2^3 + t^7.02/g2^15 + (g2^12*t^7.29)/g1^6 + (g2^11*t^7.31)/g1^3 + 2*g2^10*t^7.32 + 2*g1^3*g2^9*t^7.33 + g1^6*g2^8*t^7.34 + t^7.39/(g1^3*g2^2) + (2*t^7.4)/g2^3 + t^7.49/g2^16 + (3*g2^10*t^7.77)/g1^3 + g2^9*t^7.79 + 2*g1^3*g2^8*t^7.8 + (2*t^7.87)/g2^4 + (g1^3*t^7.88)/g2^5 + (2*t^7.96)/g2^17 + (2*g2^10*t^8.23)/g1^6 + (g2^9*t^8.24)/g1^3 + 4*g2^8*t^8.25 + g1^3*g2^7*t^8.27 + g1^6*g2^6*t^8.28 - t^8.32/(g1^6*g2^3) + t^8.33/(g1^3*g2^4) - (2*t^8.34)/g2^5 + (g1^3*t^8.35)/g2^6 + (2*t^8.43)/g2^18 + g2^20*t^8.64 + g1^6*g2^18*t^8.66 + (g2^9*t^8.7)/g1^6 + (3*g2^8*t^8.71)/g1^3 + g2^7*t^8.72 + 3*g1^3*g2^6*t^8.73 + t^8.81/g2^6 + (2*t^8.89)/g2^19 + t^8.81/(g2^6*y^2) - t^3.94/(g2^2*y) - t^4.87/(g2^4*y) - t^6.28/(g2^7*y) - t^6.75/(g2^8*y) - (g2^5*t^7.12)/(g1^3*y) - (g1^3*g2^3*t^7.14)/y - (2*t^7.21)/(g2^9*y) - t^7.68/(g2^10*y) - (g2^3*t^8.05)/(g1^3*y) - (g1^3*g2*t^8.08)/y + (g2^2*t^8.52)/(g1^3*y) - (g2*t^8.53)/y + (g1^3*t^8.54)/y - (t^3.94*y)/g2^2 - (t^4.87*y)/g2^4 - (t^6.28*y)/g2^7 - (t^6.75*y)/g2^8 - (g2^5*t^7.12*y)/g1^3 - g1^3*g2^3*t^7.14*y - (2*t^7.21*y)/g2^9 - (t^7.68*y)/g2^10 - (g2^3*t^8.05*y)/g1^3 - g1^3*g2*t^8.08*y + (g2^2*t^8.52*y)/g1^3 - g2*t^8.53*y + g1^3*t^8.54*y + (t^8.81*y^2)/g2^6 |
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 |
---|---|---|---|---|---|---|---|---|---|
57302 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1.4334 | 1.623 | 0.8832 | [X:[1.3613], M:[0.7984], q:[0.4354, 0.5847], qb:[0.4469, 0.6169], phi:[0.3194]] | t^2.395 + t^2.647 + t^2.874 + t^3.095 + t^3.157 + t^3.605 + t^4.053 + t^4.084 + t^4.115 + 2*t^4.563 + t^4.79 + t^5.011 + t^5.042 + t^5.073 + t^5.269 + t^5.293 + t^5.324 + t^5.49 + 2*t^5.521 + t^5.741 + t^5.748 + t^5.773 + t^5.804 + t^5.969 - 2*t^6. - t^3.958/y - t^4.916/y - t^3.958*y - t^4.916*y | detail |