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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79653 | Sp2s2nf1 | ${}M_{1}S_{1}S_{2}$ + ${ }M_{2}S_{1}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{2}M_{3}$ + ${ }q_{1}^{2}S_{1}$ | 2.2994 | 2.382 | 0.9653 | [X:[], M:[0.9119, 1.0881, 0.9119], q:[0.772, 0.6993], qb:[], phi:[], S:[0.4559, 0.6322], Sb:[], A:[], Ab:[]] | [X:[], M:[[-4], [4], [-4]], q:[[1], [-25]], qb:[], phi:[], S:[[-2], [6]], Sb:[], A:[], Ab:[]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }M_{3}$, ${ }S_{2}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }S_{1}^{4}$, ${ }q_{2}^{2}S_{1}$ | ${}S_{1}^{3}S_{2}$ | -1 | 2*t^2.736 + t^3.793 + t^4.414 + 3*t^5.471 + t^5.564 - t^6. + t^6.092 - t^6.218 + t^6.311 + 4*t^6.529 + t^7.057 + 2*t^7.15 - t^7.368 + t^7.46 + 2*t^7.586 + t^7.678 + t^7.804 - t^7.896 - t^8.115 + 5*t^8.207 + 2*t^8.299 - t^8.518 - 4*t^8.736 + 4*t^8.828 - 2*t^8.954 - t^4.368/y - t^4.896/y - (2*t^7.104)/y - (2*t^7.632)/y - (2*t^8.161)/y + t^8.471/y - (2*t^8.689)/y - t^8.782/y - t^4.368*y - t^4.896*y - 2*t^7.104*y - 2*t^7.632*y - 2*t^8.161*y + t^8.471*y - 2*t^8.689*y - t^8.782*y | (2*t^2.736)/g1^4 + g1^12*t^3.793 + t^4.414/g1^24 + (3*t^5.471)/g1^8 + t^5.564/g1^52 - t^6. + t^6.092/g1^44 - g1^26*t^6.218 + t^6.311/g1^18 + 4*g1^8*t^6.529 + g1^16*t^7.057 + (2*t^7.15)/g1^28 - t^7.368/g1^2 + t^7.46/g1^46 + 2*g1^24*t^7.586 + t^7.678/g1^20 + g1^50*t^7.804 - g1^6*t^7.896 - g1^32*t^8.115 + (5*t^8.207)/g1^12 + (2*t^8.299)/g1^56 - t^8.518/g1^30 - (4*t^8.736)/g1^4 + (4*t^8.828)/g1^48 - 2*g1^22*t^8.954 - t^4.368/(g1^2*y) - (g1^6*t^4.896)/y - (2*t^7.104)/(g1^6*y) - (2*g1^2*t^7.632)/y - (2*g1^10*t^8.161)/y + t^8.471/(g1^8*y) - (2*g1^18*t^8.689)/y - t^8.782/(g1^26*y) - (t^4.368*y)/g1^2 - g1^6*t^4.896*y - (2*t^7.104*y)/g1^6 - 2*g1^2*t^7.632*y - 2*g1^10*t^8.161*y + (t^8.471*y)/g1^8 - 2*g1^18*t^8.689*y - (t^8.782*y)/g1^26 |
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 |
---|---|---|---|---|---|---|---|---|---|
79585 | Sp2s2nf1 | ${}M_{1}S_{1}S_{2}$ + ${ }M_{2}S_{1}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{2}M_{3}$ | 2.3038 | 2.3948 | 0.962 | [X:[], M:[0.9029, 1.0971, 0.9029], q:[0.7087, 0.7087], qb:[], phi:[], S:[0.4515, 0.6456], Sb:[], A:[], Ab:[]] | 2*t^2.709 + t^3.874 + t^4.252 + 3*t^5.417 + 3*t^5.607 - 4*t^6. - t^4.354/y - t^4.937/y - t^4.354*y - t^4.937*y | detail |