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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46018 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.5498 | 0.6599 | 0.8332 | [M:[1.0566, 0.9434], q:[0.5283, 0.4152], qb:[0.5283, 1.1195], phi:[0.3522]] | [M:[[-6], [6]], q:[[-3], [9]], qb:[[-3], [5]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}\phi_{1}^{2}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$ | ${}\phi_{1}^{3}q_{2}\tilde{q}_{1}$ | -1 | t^2.113 + 2*t^2.83 + t^3.17 + t^3.548 + t^3.887 + 2*t^4.226 + t^4.604 + 3*t^4.943 + 3*t^5.661 - t^6. + t^6.339 + 2*t^6.378 + t^6.717 + 2*t^7.057 + t^7.095 + 2*t^7.434 + 3*t^7.774 - 2*t^8.113 + t^8.152 + 2*t^8.452 + 4*t^8.491 - 4*t^8.83 - t^4.057/y - t^6.17/y + (3*t^7.943)/y + (2*t^8.661)/y - t^4.057*y - t^6.17*y + 3*t^7.943*y + 2*t^8.661*y | t^2.113/g1^4 + 2*g1^6*t^2.83 + t^3.17/g1^6 + g1^16*t^3.548 + g1^4*t^3.887 + (2*t^4.226)/g1^8 + g1^14*t^4.604 + 3*g1^2*t^4.943 + 3*g1^12*t^5.661 - t^6. + t^6.339/g1^12 + 2*g1^22*t^6.378 + g1^10*t^6.717 + (2*t^7.057)/g1^2 + g1^32*t^7.095 + 2*g1^20*t^7.434 + 3*g1^8*t^7.774 - (2*t^8.113)/g1^4 + g1^30*t^8.152 + (2*t^8.452)/g1^16 + 4*g1^18*t^8.491 - 4*g1^6*t^8.83 - t^4.057/(g1^2*y) - t^6.17/(g1^6*y) + (3*g1^2*t^7.943)/y + (2*g1^12*t^8.661)/y - (t^4.057*y)/g1^2 - (t^6.17*y)/g1^6 + 3*g1^2*t^7.943*y + 2*g1^12*t^8.661*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 |
---|---|---|---|---|---|---|---|---|---|
45932 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ | 0.57 | 0.6943 | 0.8211 | [M:[1.0, 1.0], q:[0.5963, 0.4037], qb:[0.4037, 1.0062], phi:[0.3975]] | 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. - t^4.193/y - t^4.193*y | detail |