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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79674 | Sp2s2nf1 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{1}S_{1}S_{2}$ + ${ }M_{2}S_{1}S_{2}$ + ${ }M_{3}S_{1}^{2}$ + ${ }M_{3}^{2}$ | 2.3683 | 2.5112 | 0.9431 | [X:[], M:[0.8571, 0.8571, 1.0], q:[0.5714, 0.5714], qb:[], phi:[], S:[0.5, 0.6429], Sb:[], A:[], Ab:[]] | [X:[], M:[[0], [0], [0]], q:[[-1], [1]], qb:[], phi:[], S:[[0], [0]], Sb:[], A:[], Ab:[]] | 1 | {a: 25995/10976, c: 27563/10976, M1: 6/7, M2: 6/7, M3: 1, q1: 4/7, q2: 4/7, S1: 1/2, S2: 9/14} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{1}$, ${ }M_{2}$, ${ }M_{3}$, ${ }S_{2}^{2}$, ${ }q_{1}^{2}S_{1}$, ${ }q_{1}q_{2}S_{1}$, ${ }q_{2}^{2}S_{1}$, ${ }q_{1}^{2}S_{1}$, ${ }q_{2}^{2}S_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}^{2}$, ${ }q_{1}^{2}S_{2}$, ${ }q_{1}q_{2}S_{2}$, ${ }q_{2}^{2}S_{2}$, ${ }q_{1}^{2}S_{2}$, ${ }q_{2}^{2}S_{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{3}$ | ${}S_{1}^{4}$ | -3 | 2*t^2.571 + t^3. + t^3.857 + 3*t^4.929 + 3*t^5.143 + 3*t^5.357 + t^5.571 - 3*t^6. + 3*t^6.429 + 7*t^6.857 + 2*t^7.286 - t^7.5 + 6*t^7.714 + 5*t^7.929 + t^8.143 + 10*t^8.357 - 4*t^8.571 + 10*t^8.786 - t^4.5/y - t^4.929/y - t^7.071/y - (3*t^7.5)/y - (2*t^7.929)/y + t^8.143/y - (2*t^8.357)/y + (2*t^8.571)/y - (2*t^8.786)/y - t^4.5*y - t^4.929*y - t^7.071*y - 3*t^7.5*y - 2*t^7.929*y + t^8.143*y - 2*t^8.357*y + 2*t^8.571*y - 2*t^8.786*y | 2*t^2.571 + t^3. + t^3.857 + t^4.929 + t^4.929/g1^2 + g1^2*t^4.929 + 3*t^5.143 + t^5.357 + t^5.357/g1^2 + g1^2*t^5.357 + t^5.571 - t^6. - t^6./g1^2 - g1^2*t^6. + 3*t^6.429 + 5*t^6.857 + t^6.857/g1^2 + g1^2*t^6.857 + 2*t^7.286 - t^7.5 + 6*t^7.714 + t^7.929 + (2*t^7.929)/g1^2 + 2*g1^2*t^7.929 + t^8.143 + 4*t^8.357 + (3*t^8.357)/g1^2 + 3*g1^2*t^8.357 - 2*t^8.571 - t^8.571/g1^2 - g1^2*t^8.571 + 4*t^8.786 + (3*t^8.786)/g1^2 + 3*g1^2*t^8.786 - t^4.5/y - t^4.929/y - t^7.071/y - (3*t^7.5)/y - (2*t^7.929)/y + t^8.143/y - (2*t^8.357)/y + (2*t^8.571)/y - (2*t^8.786)/y - t^4.5*y - t^4.929*y - t^7.071*y - 3*t^7.5*y - 2*t^7.929*y + t^8.143*y - 2*t^8.357*y + 2*t^8.571*y - 2*t^8.786*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 |
---|---|---|---|---|---|---|---|---|---|
79567 | Sp2s2nf1 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{1}S_{1}S_{2}$ + ${ }M_{2}S_{1}S_{2}$ + ${ }M_{3}S_{1}^{2}$ | 2.4186 | 2.5716 | 0.9405 | [X:[], M:[0.8571, 0.8571, 0.8374], q:[0.5714, 0.5714], qb:[], phi:[], S:[0.5813, 0.5616], Sb:[], A:[], Ab:[]] | t^2.512 + 2*t^2.571 + t^3.369 + t^5.024 + 2*t^5.084 + 3*t^5.113 + 3*t^5.143 + 3*t^5.172 + t^5.881 + t^5.941 - 5*t^6. - t^4.685/y - t^4.744/y - t^4.685*y - t^4.744*y | detail |