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 |
---|---|---|---|---|---|---|---|---|---|
2775 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}X_{1}$ + ${ }M_{1}M_{5}$ | 0.5999 | 0.7213 | 0.8316 | [X:[1.6114], M:[0.7772, 1.1658, 0.3886, 0.8342, 1.2228], q:[0.4457, 0.7772], qb:[0.3886, 0.8342], phi:[0.3886]] | [X:[[1]], M:[[-2], [-3], [-1], [3], [2]], q:[[4], [-2]], qb:[[-1], [3]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | ${}M_{5}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ | 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 | t^2.332/g1^2 + g1^3*t^2.503 + (2*t^3.497)/g1^3 + 3*g1^2*t^3.668 + 2*g1^7*t^3.84 + t^4.663/g1^4 + 2*g1*t^4.834 + g1^6*t^5.005 + 3*g1^5*t^6.171 + 2*g1^10*t^6.342 + (2*t^6.995)/g1^6 + (2*t^7.166)/g1 + 5*g1^4*t^7.337 + 5*g1^9*t^7.508 + 3*g1^14*t^7.679 - t^8.332/g1^2 - g1^3*t^8.503 + 3*g1^8*t^8.674 + 2*g1^13*t^8.845 - t^4.166/(g1*y) - t^6.497/(g1^3*y) + (2*g1*t^7.834)/y + t^8.829/(g1^5*y) - (t^4.166*y)/g1 - (t^6.497*y)/g1^3 + 2*g1*t^7.834*y + (t^8.829*y)/g1^5 |
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 |
---|---|---|---|---|---|---|---|---|---|
1774 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}X_{1}$ | 0.6178 | 0.7527 | 0.8207 | [X:[1.6138], M:[0.7725, 1.1587, 0.3862, 0.8413], q:[0.455, 0.7725], qb:[0.3862, 0.8413], 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 |