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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57795 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ | 1.411 | 1.5985 | 0.8827 | [X:[1.4286], M:[0.7143, 0.7143], q:[0.5595, 0.5595], qb:[0.4405, 0.7262], phi:[0.2857]] | [X:[[0, 0]], M:[[-1, -1], [1, 1]], q:[[-1, -2], [1, 0]], qb:[[0, 1], [0, 1]], phi:[[0, 0]]] | 2 | {a: 61947/43904, c: 70179/43904, X1: 10/7, M1: 5/7, M2: 5/7, q1: 47/84, q2: 47/84, qb1: 37/84, qb2: 61/84, phi1: 2/7} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }M_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}^{2}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{6}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$ | ${}M_{2}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$ | 0 | 2*t^2.14 + t^2.57 + 2*t^3. + 2*t^3.86 + 4*t^4.29 + 6*t^4.71 + 4*t^5.14 + 4*t^5.57 + t^5.68 + 2*t^5.89 + 8*t^6.43 + 3*t^6.54 + 2*t^6.75 + 9*t^6.86 - t^7.18 + 12*t^7.29 + 2*t^7.39 + 4*t^7.61 + 14*t^7.71 - 2*t^7.82 - t^8.04 + 2*t^8.14 + 2*t^8.25 + 2*t^8.46 + 20*t^8.57 + 2*t^8.68 + t^8.57/y^2 - t^3.86/y - t^4.71/y - (2*t^6.)/y - t^6.43/y - (4*t^6.86)/y + t^8.14/y - (2*t^8.57)/y - t^3.86*y - t^4.71*y - 2*t^6.*y - t^6.43*y - 4*t^6.86*y + t^8.14*y - 2*t^8.57*y + t^8.57*y^2 | t^2.14/(g1*g2) + g1*g2*t^2.14 + t^2.57 + t^3./(g1*g2) + g1*g2*t^3. + t^3.86/(g1*g2) + g1*g2*t^3.86 + 2*t^4.29 + t^4.29/(g1^2*g2^2) + g1^2*g2^2*t^4.29 + (3*t^4.71)/(g1*g2) + 3*g1*g2*t^4.71 + 2*t^5.14 + t^5.14/(g1^2*g2^2) + g1^2*g2^2*t^5.14 + (2*t^5.57)/(g1*g2) + 2*g1*g2*t^5.57 + g2^3*t^5.68 + t^5.89/(g1*g2^4) + (g1*t^5.89)/g2^2 - 2*t^6. + t^6./(g1^2*g2^2) + g1^2*g2^2*t^6. + t^6.43/(g1^3*g2^3) + (3*t^6.43)/(g1*g2) + 3*g1*g2*t^6.43 + g1^3*g2^3*t^6.43 + 3*g2^3*t^6.54 + t^6.75/(g1*g2^4) + (g1*t^6.75)/g2^2 + 3*t^6.86 + (3*t^6.86)/(g1^2*g2^2) + 3*g1^2*g2^2*t^6.86 - t^7.18/g2^3 + t^7.29/(g1^3*g2^3) + (5*t^7.29)/(g1*g2) + 5*g1*g2*t^7.29 + g1^3*g2^3*t^7.29 + 2*g2^3*t^7.39 + g1^3*t^7.61 + t^7.61/(g1^3*g2^6) + t^7.61/(g1*g2^4) + (g1*t^7.61)/g2^2 + 6*t^7.71 + (4*t^7.71)/(g1^2*g2^2) + 4*g1^2*g2^2*t^7.71 - (g2^2*t^7.82)/g1 - g1*g2^4*t^7.82 - t^8.04/g2^3 + t^8.14/(g1^3*g2^3) + g1^3*g2^3*t^8.14 + 2*g2^3*t^8.25 + t^8.46/(g1*g2^4) + (g1*t^8.46)/g2^2 + 6*t^8.57 + t^8.57/(g1^4*g2^4) + (6*t^8.57)/(g1^2*g2^2) + 6*g1^2*g2^2*t^8.57 + g1^4*g2^4*t^8.57 + (g2^2*t^8.68)/g1 + g1*g2^4*t^8.68 + t^8.57/y^2 - t^3.86/y - t^4.71/y - t^6./(g1*g2*y) - (g1*g2*t^6.)/y - t^6.43/y - (2*t^6.86)/(g1*g2*y) - (2*g1*g2*t^6.86)/y + t^8.14/y - t^8.57/(g1*g2*y) - (g1*g2*t^8.57)/y - t^3.86*y - t^4.71*y - (t^6.*y)/(g1*g2) - g1*g2*t^6.*y - t^6.43*y - (2*t^6.86*y)/(g1*g2) - 2*g1*g2*t^6.86*y + t^8.14*y - (t^8.57*y)/(g1*g2) - g1*g2*t^8.57*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 |
---|---|---|---|---|---|---|---|---|---|
57286 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$ | 1.4759 | 1.6818 | 0.8775 | [X:[1.3442], M:[0.9514, 0.6882], q:[0.4921, 0.5242], qb:[0.4919, 0.5244], phi:[0.3279]] | t^2.064 + t^2.854 + t^2.951 + t^2.952 + t^3.048 + t^3.049 + t^4.032 + 2*t^4.033 + t^4.129 + t^4.13 + 2*t^4.919 + 3*t^5.016 + t^5.017 + 2*t^5.113 + t^5.114 + t^5.508 + t^5.509 + t^5.605 + t^5.606 + t^5.708 + t^5.805 + t^5.806 + t^5.902 + t^5.903 + t^5.904 + t^5.999 - 3*t^6. - t^3.984/y - t^4.967/y - t^3.984*y - t^4.967*y | detail |