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 |
---|---|---|---|---|---|---|---|---|---|
59043 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}X_{2}$ | 0.9042 | 1.0292 | 0.8785 | [X:[1.4286, 1.4286], M:[], q:[0.4762, 0.7619], qb:[0.9524, 0.0952], phi:[0.2857]] | [X:[[0], [0]], M:[], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 2481/2744, c: 353/343, X1: 10/7, X2: 10/7, q1: 10/21, q2: 16/21, qb1: 20/21, qb2: 2/21, phi1: 2/7} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }X_{1}$, ${ }X_{2}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{6}\tilde{q}_{2}^{3}$, ${ }\phi_{1}^{4}q_{1}\tilde{q}_{2}^{4}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}^{4}$ | 3 | 3*t^2.57 + 2*t^3.43 + 4*t^4.29 + 6*t^5.14 + 3*t^6. + 9*t^6.86 + 11*t^7.71 + 8*t^8.57 + t^8.57/y^2 - t^3.86/y - t^4.71/y - (2*t^6.43)/y - (2*t^7.29)/y + t^8.14/y - t^3.86*y - t^4.71*y - 2*t^6.43*y - 2*t^7.29*y + t^8.14*y + t^8.57*y^2 | 3*t^2.57 + 2*t^3.43 + 4*t^4.29 + 6*t^5.14 + 3*t^6. + 9*t^6.86 + 11*t^7.71 + 8*t^8.57 + t^8.57/y^2 - t^3.86/y - t^4.71/y - (2*t^6.43)/y - (2*t^7.29)/y + t^8.14/y - t^3.86*y - t^4.71*y - 2*t^6.43*y - 2*t^7.29*y + t^8.14*y + t^8.57*y^2 |
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 |
---|---|---|---|---|---|---|---|---|---|
57630 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | 1.3191 | 1.4708 | 0.8968 | [X:[1.4286], M:[], q:[0.6508, 0.4127], qb:[0.7778, 0.4444], phi:[0.2857]] | 2*t^2.57 + t^3.29 + t^3.43 + t^3.57 + t^4.14 + 3*t^4.29 + t^4.43 + 4*t^5.14 + t^5.29 + 2*t^5.86 - t^3.86/y - t^4.71/y - t^3.86*y - t^4.71*y | detail | {a: 7239/5488, c: 1009/686, X1: 10/7, q1: 41/63, q2: 26/63, qb1: 7/9, qb2: 4/9, phi1: 2/7} |