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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60940 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1.1792 | 1.344 | 0.8774 | [X:[1.2727, 1.4545], M:[1.2727], q:[0.7273, 0.1818], qb:[0.5455, 0.3636], phi:[0.3636]] | [X:[[0], [0]], M:[[0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 2283/1936, c: 1301/968, X1: 14/11, X2: 16/11, M1: 14/11, q1: 8/11, q2: 2/11, qb1: 6/11, qb2: 4/11, phi1: 4/11} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$ | 2 | t^2.73 + 3*t^3.27 + 4*t^3.82 + 3*t^4.36 + 3*t^4.91 + 2*t^5.45 + 2*t^6. + 7*t^6.55 + 10*t^7.09 + 13*t^7.64 + 13*t^8.18 + 9*t^8.73 - t^4.09/y - t^5.18/y - (2*t^7.36)/y - (3*t^7.91)/y - (3*t^8.45)/y - t^4.09*y - t^5.18*y - 2*t^7.36*y - 3*t^7.91*y - 3*t^8.45*y | t^2.73 + 3*t^3.27 + 4*t^3.82 + 3*t^4.36 + 3*t^4.91 + 2*t^5.45 + 2*t^6. + 7*t^6.55 + 10*t^7.09 + 13*t^7.64 + 13*t^8.18 + 9*t^8.73 - t^4.09/y - t^5.18/y - (2*t^7.36)/y - (3*t^7.91)/y - (3*t^8.45)/y - t^4.09*y - t^5.18*y - 2*t^7.36*y - 3*t^7.91*y - 3*t^8.45*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 |
---|---|---|---|---|---|---|---|---|---|
58568 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ | 1.1832 | 1.3524 | 0.8749 | [X:[1.2584, 1.4831], M:[1.2584], q:[0.7154, 0.1985], qb:[0.5431, 0.3184], phi:[0.3708]] | t^2.66 + t^3.1 + 2*t^3.34 + 4*t^3.78 + t^4.21 + 2*t^4.45 + t^4.65 + t^4.89 + t^5.12 + 2*t^5.33 + 2*t^5.76 - t^4.11/y - t^5.22/y - t^4.11*y - t^5.22*y | detail |