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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113 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$ + ${ }M_{1}^{2}$ | 0.57 | 0.6943 | 0.8211 | [M:[1.0], q:[0.5963, 1.0062], qb:[0.4037, 0.4037], phi:[0.3975]] | [M:[[0]], q:[[-3], [5]], qb:[[3], [3]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ | 1 | t^2.385 + t^2.422 + 2*t^3. + 3*t^3.615 + 2*t^4.23 + t^4.77 + 2*t^4.807 + t^4.845 + 2*t^5.422 + t^6. + 3*t^6.037 - 2*t^6.578 + 4*t^6.615 + 2*t^6.652 + t^7.155 - 2*t^7.193 + 7*t^7.23 + t^7.267 - 2*t^7.807 + 6*t^7.845 - 2*t^8.385 + 6*t^8.46 - t^4.193/y - t^6.578/y + (2*t^7.807)/y + (2*t^8.385)/y + (2*t^8.422)/y - t^8.963/y - t^4.193*y - t^6.578*y + 2*t^7.807*y + 2*t^8.385*y + 2*t^8.422*y - t^8.963*y | t^2.385/g1^4 + g1^6*t^2.422 + 2*t^3. + 3*g1^4*t^3.615 + 2*g1^8*t^4.23 + t^4.77/g1^8 + 2*g1^2*t^4.807 + g1^12*t^4.845 + 2*g1^6*t^5.422 + t^6. + 3*g1^10*t^6.037 - (2*t^6.578)/g1^6 + 4*g1^4*t^6.615 + 2*g1^14*t^6.652 + t^7.155/g1^12 - (2*t^7.193)/g1^2 + 7*g1^8*t^7.23 + g1^18*t^7.267 - 2*g1^2*t^7.807 + 6*g1^12*t^7.845 - (2*t^8.385)/g1^4 + 6*g1^16*t^8.46 - t^4.193/(g1^2*y) - t^6.578/(g1^6*y) + (2*g1^2*t^7.807)/y + (2*t^8.385)/(g1^4*y) + (2*g1^6*t^8.422)/y - t^8.963/(g1^10*y) - (t^4.193*y)/g1^2 - (t^6.578*y)/g1^6 + 2*g1^2*t^7.807*y + (2*t^8.385*y)/g1^4 + 2*g1^6*t^8.422*y - (t^8.963*y)/g1^10 |
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 |
---|---|---|---|---|---|---|---|---|---|
75 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$ | 0.6281 | 0.758 | 0.8286 | [M:[0.6967], q:[0.8359, 0.809], qb:[0.4674, 0.4674], phi:[0.3551]] | t^2.09 + t^2.13 + t^2.805 + 2*t^3.829 + 3*t^3.87 + t^3.91 + t^4.18 + t^4.22 + t^4.261 + t^4.895 + 2*t^4.935 + t^5.609 + 2*t^5.919 + 3*t^5.96 - t^6. - t^4.065/y - t^4.065*y | detail |