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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79586 | Sp2s2nf1 | ${}q_{1}^{2}S_{2}$ + ${ }M_{1}S_{1}S_{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }M_{1}S_{1}^{2}$ | 2.4051 | 2.5304 | 0.9505 | [X:[], M:[0.8883, 0.67], q:[0.7221, 0.6079], qb:[], phi:[], S:[0.5558, 0.5558], Sb:[], A:[], Ab:[]] | [X:[], M:[[-4], [24]], q:[[-1], [-23]], qb:[], phi:[], S:[[2], [2]], Sb:[], A:[], Ab:[]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{1}$, ${ }S_{1}^{2}$, ${ }S_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }q_{2}^{2}S_{1}$, ${ }q_{2}^{2}S_{2}$, ${ }M_{1}^{2}$, ${ }M_{2}S_{1}^{2}$, ${ }M_{2}S_{2}^{2}$, ${ }q_{1}q_{2}S_{1}$ | ${}$ | -1 | t^2.01 + t^2.665 + 2*t^3.335 + t^4.02 + t^4.675 + 2*t^5.315 + t^5.33 + 2*t^5.345 + t^5.657 - t^6. + t^6.03 - t^6.343 + 9*t^6.67 + t^6.685 + t^6.982 + 4*t^7.325 + t^7.34 + 2*t^7.355 - t^7.668 + t^7.995 - 2*t^8.01 + t^8.04 - t^8.322 + 10*t^8.65 - 2*t^8.665 + 9*t^8.68 + t^8.695 + 7*t^8.992 - (2*t^4.668)/y - (2*t^6.678)/y + t^7.675/y - (8*t^8.003)/y + (2*t^8.345)/y - (2*t^8.688)/y - 2*t^4.668*y - 2*t^6.678*y + t^7.675*y - 8*t^8.003*y + 2*t^8.345*y - 2*t^8.688*y | g1^24*t^2.01 + t^2.665/g1^4 + 2*g1^4*t^3.335 + g1^48*t^4.02 + g1^20*t^4.675 + (2*t^5.315)/g1^44 + t^5.33/g1^8 + 2*g1^28*t^5.345 + t^5.657/g1^22 - t^6. + g1^72*t^6.03 - g1^22*t^6.343 + 9*g1^8*t^6.67 + g1^44*t^6.685 + t^6.982/g1^42 + (4*t^7.325)/g1^20 + g1^16*t^7.34 + 2*g1^52*t^7.355 - g1^2*t^7.668 + t^7.995/g1^12 - 2*g1^24*t^8.01 + g1^96*t^8.04 - t^8.322/g1^26 + (10*t^8.65)/g1^40 - (2*t^8.665)/g1^4 + 9*g1^32*t^8.68 + g1^68*t^8.695 + (7*t^8.992)/g1^18 - (2*g1^2*t^4.668)/y - (2*g1^26*t^6.678)/y + (g1^20*t^7.675)/y - (8*g1^6*t^8.003)/y + (2*g1^28*t^8.345)/y - (2*g1^50*t^8.688)/y - 2*g1^2*t^4.668*y - 2*g1^26*t^6.678*y + g1^20*t^7.675*y - 8*g1^6*t^8.003*y + 2*g1^28*t^8.345*y - 2*g1^50*t^8.688*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 |
---|---|---|---|---|---|---|---|---|---|
79499 | Sp2s2nf1 | ${}q_{1}^{2}S_{2}$ + ${ }M_{1}S_{1}S_{2}$ + ${ }M_{2}q_{1}q_{2}$ | 2.4056 | 2.5313 | 0.9504 | [X:[], M:[0.8878, 0.6733], q:[0.7178, 0.6088], qb:[], phi:[], S:[0.5478, 0.5644], Sb:[], A:[], Ab:[]] | t^2.02 + t^2.663 + t^3.287 + t^3.386 + t^4.04 + t^4.683 + t^5.297 + t^5.307 + t^5.327 + t^5.346 + t^5.406 + t^5.624 + t^5.95 - 2*t^6. - t^4.644/y - t^4.693/y - t^4.644*y - t^4.693*y | detail |