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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978 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}M_{6}$ | 0.71 | 0.8716 | 0.8146 | [M:[0.8862, 1.0, 0.8862, 1.0, 1.0569, 0.9431], q:[0.6422, 0.4716], qb:[0.4716, 0.5284], phi:[0.4716]] | [M:[[1, -3], [-1, -1], [-1, -5], [1, 1], [0, 2], [0, -2]], q:[[0, 5], [-1, -2]], qb:[[1, 0], [0, 1]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }M_{1}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$ | ${}M_{2}^{2}$, ${ }M_{4}^{2}$ | -3 | 2*t^2.659 + 2*t^2.829 + 2*t^3. + t^3.512 + 3*t^4.244 + 2*t^4.415 + t^4.585 + 2*t^4.756 + t^4.927 + t^5.268 + 3*t^5.317 + 2*t^5.488 + 6*t^5.659 + 2*t^5.829 - 3*t^6. + 4*t^6.903 + t^7.024 + 9*t^7.073 + 8*t^7.244 + t^7.415 + 2*t^7.585 + 2*t^7.756 + 4*t^7.976 + t^8.097 + 3*t^8.147 + 2*t^8.268 + 6*t^8.317 + 9*t^8.488 + t^8.78 - 6*t^8.829 - t^4.415/y - (2*t^7.073)/y - t^7.244/y + t^7.585/y + (2*t^7.756)/y + t^8.317/y + (4*t^8.488)/y + (5*t^8.659)/y + (4*t^8.829)/y - t^4.415*y - 2*t^7.073*y - t^7.244*y + t^7.585*y + 2*t^7.756*y + t^8.317*y + 4*t^8.488*y + 5*t^8.659*y + 4*t^8.829*y | t^2.659/(g1*g2^5) + (g1*t^2.659)/g2^3 + (2*t^2.829)/g2^2 + t^3./(g1*g2) + g1*g2*t^3. + g2^6*t^3.512 + t^4.244/(g1^2*g2^5) + t^4.244/g2^3 + (g1^2*t^4.244)/g2 + g1*t^4.415 + t^4.415/(g1*g2^2) + g2*t^4.585 + (g2^2*t^4.756)/g1 + g1*g2^4*t^4.756 + g2^5*t^4.927 + g2^9*t^5.268 + t^5.317/(g1^2*g2^10) + t^5.317/g2^8 + (g1^2*t^5.317)/g2^6 + t^5.488/(g1*g2^7) + (g1*t^5.488)/g2^5 + t^5.659/(g1^2*g2^6) + (4*t^5.659)/g2^4 + (g1^2*t^5.659)/g2^2 + t^5.829/(g1*g2^3) + (g1*t^5.829)/g2 - 3*t^6. + t^6.903/(g1^3*g2^10) + t^6.903/(g1*g2^8) + (g1*t^6.903)/g2^6 + (g1^3*t^6.903)/g2^4 + g2^12*t^7.024 + (3*t^7.073)/(g1^2*g2^7) + (3*t^7.073)/g2^5 + (3*g1^2*t^7.073)/g2^3 + g1^3*t^7.244 + t^7.244/(g1^3*g2^6) + (3*t^7.244)/(g1*g2^4) + (3*g1*t^7.244)/g2^2 + t^7.415/g2 + t^7.585/g1 + g1*g2^2*t^7.585 + (g2*t^7.756)/g1^2 + g1^2*g2^5*t^7.756 + t^7.976/(g1^3*g2^15) + t^7.976/(g1*g2^13) + (g1*t^7.976)/g2^11 + (g1^3*t^7.976)/g2^9 + g2^7*t^8.097 + t^8.147/(g1^2*g2^12) + t^8.147/g2^10 + (g1^2*t^8.147)/g2^8 + (g2^8*t^8.268)/g1 + g1*g2^10*t^8.268 + t^8.317/(g1^3*g2^11) + (2*t^8.317)/(g1*g2^9) + (2*g1*t^8.317)/g2^7 + (g1^3*t^8.317)/g2^5 + t^8.488/(g1^4*g2^10) + t^8.488/(g1^2*g2^8) + (5*t^8.488)/g2^6 + (g1^2*t^8.488)/g2^4 + (g1^4*t^8.488)/g2^2 + t^8.659/(g1^3*g2^7) - t^8.659/(g1*g2^5) - (g1*t^8.659)/g2^3 + (g1^3*t^8.659)/g2 + g2^15*t^8.78 - (6*t^8.829)/g2^2 - t^4.415/(g2*y) - t^7.073/(g1*g2^6*y) - (g1*t^7.073)/(g2^4*y) - t^7.244/(g2^3*y) + (g2*t^7.585)/y + (g2^2*t^7.756)/(g1*y) + (g1*g2^4*t^7.756)/y + t^8.317/(g2^8*y) + (2*t^8.488)/(g1*g2^7*y) + (2*g1*t^8.488)/(g2^5*y) + t^8.659/(g1^2*g2^6*y) + (3*t^8.659)/(g2^4*y) + (g1^2*t^8.659)/(g2^2*y) + (2*t^8.829)/(g1*g2^3*y) + (2*g1*t^8.829)/(g2*y) - (t^4.415*y)/g2 - (t^7.073*y)/(g1*g2^6) - (g1*t^7.073*y)/g2^4 - (t^7.244*y)/g2^3 + g2*t^7.585*y + (g2^2*t^7.756*y)/g1 + g1*g2^4*t^7.756*y + (t^8.317*y)/g2^8 + (2*t^8.488*y)/(g1*g2^7) + (2*g1*t^8.488*y)/g2^5 + (t^8.659*y)/(g1^2*g2^6) + (3*t^8.659*y)/g2^4 + (g1^2*t^8.659*y)/g2^2 + (2*t^8.829*y)/(g1*g2^3) + (2*g1*t^8.829*y)/g2 |
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 |
---|---|---|---|---|---|---|---|---|---|
606 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ | 0.7051 | 0.8629 | 0.8172 | [M:[0.9027, 1.0, 0.9027, 1.0, 1.0486], q:[0.6216, 0.4757], qb:[0.4757, 0.5243], phi:[0.4757]] | 2*t^2.708 + t^2.854 + 2*t^3. + t^3.146 + t^3.438 + 3*t^4.281 + 2*t^4.427 + t^4.573 + 2*t^4.719 + t^4.865 + t^5.157 + 3*t^5.416 + 4*t^5.708 + 2*t^5.854 - 2*t^6. - t^4.427/y - t^4.427*y | detail |