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 |
---|---|---|---|---|---|---|---|---|---|
46795 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}^{2}$ | 0.5999 | 0.7213 | 0.8316 | [M:[0.7772, 1.1658, 0.8342, 1.2228], q:[0.8342, 0.3886], qb:[0.4457, 0.7772], phi:[0.3886]] | [M:[[2], [3], [-3], [-2]], q:[[-3], [1]], qb:[[-4], [2]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$ | ${}M_{1}M_{4}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0 | t^2.332 + t^2.503 + 2*t^3.497 + 3*t^3.668 + 2*t^3.84 + t^4.663 + 2*t^4.834 + t^5.005 + 3*t^6.171 + 2*t^6.342 + 2*t^6.995 + 2*t^7.166 + 5*t^7.337 + 5*t^7.508 + 3*t^7.679 - t^8.332 - t^8.503 + 3*t^8.674 + 2*t^8.845 - t^4.166/y - t^6.497/y + (2*t^7.834)/y + t^8.829/y - t^4.166*y - t^6.497*y + 2*t^7.834*y + t^8.829*y | g1^2*t^2.332 + t^2.503/g1^3 + 2*g1^3*t^3.497 + (3*t^3.668)/g1^2 + (2*t^3.84)/g1^7 + g1^4*t^4.663 + (2*t^4.834)/g1 + t^5.005/g1^6 + (3*t^6.171)/g1^5 + (2*t^6.342)/g1^10 + 2*g1^6*t^6.995 + 2*g1*t^7.166 + (5*t^7.337)/g1^4 + (5*t^7.508)/g1^9 + (3*t^7.679)/g1^14 - g1^2*t^8.332 - t^8.503/g1^3 + (3*t^8.674)/g1^8 + (2*t^8.845)/g1^13 - (g1*t^4.166)/y - (g1^3*t^6.497)/y + (2*t^7.834)/(g1*y) + (g1^5*t^8.829)/y - g1*t^4.166*y - g1^3*t^6.497*y + (2*t^7.834*y)/g1 + g1^5*t^8.829*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 |
---|---|---|---|---|---|---|---|---|---|
46307 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | 0.6178 | 0.7527 | 0.8207 | [M:[0.7725, 1.1587, 0.8413], q:[0.8413, 0.3862], qb:[0.455, 0.7725], phi:[0.3862]] | 2*t^2.317 + t^2.524 + 2*t^3.476 + 2*t^3.683 + 2*t^3.889 + 3*t^4.635 + 3*t^4.841 + t^5.048 + 2*t^5.794 + t^6. - t^4.159/y - t^4.159*y | detail |