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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58607 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ | 1.3905 | 1.5705 | 0.8854 | [X:[1.3731], M:[0.7903, 1.0905], q:[0.6667, 0.3532], qb:[0.5431, 0.5563], phi:[0.3135]] | [X:[[0, 2]], M:[[1, -5], [-1, -1]], q:[[0, 0], [0, 1]], qb:[[-1, 5], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{3}q_{2}^{3}$ | -1 | t^2.37 + t^2.69 + t^2.82 + t^3.27 + t^3.63 + 2*t^3.67 + t^4.12 + 2*t^4.57 + 2*t^4.61 + t^4.74 + t^5.06 + t^5.19 + t^5.38 + 2*t^5.51 + t^5.55 + 2*t^5.64 + t^5.87 + t^5.91 - t^6. + t^6.04 + t^6.09 + t^6.32 + 2*t^6.36 + t^6.45 + 3*t^6.49 + t^6.54 + 2*t^6.81 + t^6.85 + 2*t^6.94 + t^6.98 + t^7.11 + 3*t^7.26 + 3*t^7.3 + 3*t^7.34 + t^7.39 + t^7.43 + t^7.56 + t^7.71 + 2*t^7.75 + 2*t^7.79 + t^7.83 + t^7.84 + 2*t^7.88 + 2*t^8.01 + t^8.07 + 3*t^8.2 + 5*t^8.24 + 4*t^8.28 - 2*t^8.37 + t^8.41 + 2*t^8.46 + t^8.56 + t^8.6 + 2*t^8.73 + t^8.78 + t^8.82 + 2*t^8.86 + 2*t^8.91 + t^8.82/y^2 - t^3.94/y - t^4.88/y - t^6.31/y - t^6.63/y - t^6.76/y - t^7.21/y - t^7.25/y - t^7.57/y - t^7.61/y - t^7.7/y + t^8.06/y - t^8.15/y + t^8.19/y - (2*t^8.55)/y + t^8.64/y - t^8.68/y + t^8.96/y - t^3.94*y - t^4.88*y - t^6.31*y - t^6.63*y - t^6.76*y - t^7.21*y - t^7.25*y - t^7.57*y - t^7.61*y - t^7.7*y + t^8.06*y - t^8.15*y + t^8.19*y - 2*t^8.55*y + t^8.64*y - t^8.68*y + t^8.96*y + t^8.82*y^2 | (g1*t^2.37)/g2^5 + (g2^6*t^2.69)/g1 + t^2.82/g2^3 + t^3.27/(g1*g2) + (g2^5*t^3.63)/g1 + 2*g1*t^3.67 + g2^2*t^4.12 + (2*g2^4*t^4.57)/g1 + (2*g1*t^4.61)/g2 + (g1^2*t^4.74)/g2^10 + g2*t^5.06 + (g1*t^5.19)/g2^8 + (g2^12*t^5.38)/g1^2 + (2*g2^3*t^5.51)/g1 + (g1*t^5.55)/g2^2 + (2*t^5.64)/g2^6 + (g2^9*t^5.87)/g1 + g1*g2^4*t^5.91 - t^6. + (g1^2*t^6.04)/g2^5 + t^6.09/(g1*g2^4) + (g2^11*t^6.32)/g1^2 + 2*g2^6*t^6.36 + (g2^2*t^6.45)/g1 + (3*g1*t^6.49)/g2^3 + t^6.54/(g1^2*g2^2) + (2*g2^8*t^6.81)/g1 + g1*g2^3*t^6.85 + (2*t^6.94)/g2 + (g1^2*t^6.98)/g2^6 + (g1^3*t^7.11)/g2^15 + (3*g2^10*t^7.26)/g1^2 + 3*g2^5*t^7.3 + 3*g1^2*t^7.34 + (g2*t^7.39)/g1 + (g1*t^7.43)/g2^4 + (g1^2*t^7.56)/g2^13 + (g2^12*t^7.71)/g1^3 + (2*g2^7*t^7.75)/g1 + 2*g1*g2^2*t^7.79 + (g1^3*t^7.83)/g2^3 + (g2^3*t^7.84)/g1^2 + (2*t^7.88)/g2^2 + (2*g1*t^8.01)/g2^11 + (g2^18*t^8.07)/g1^3 + (3*g2^9*t^8.2)/g1^2 + 5*g2^4*t^8.24 + (4*g1^2*t^8.28)/g2 - (2*g1*t^8.37)/g2^5 + (g1^3*t^8.41)/g2^10 + (2*t^8.46)/g2^9 + (g2^15*t^8.56)/g1^2 + g2^10*t^8.6 + 2*g1*g2*t^8.73 + (g2^2*t^8.78)/g1^2 + t^8.82/g2^3 + (2*g1^2*t^8.86)/g2^8 + (2*t^8.91)/(g1*g2^7) + t^8.82/(g2^3*y^2) - t^3.94/(g2*y) - t^4.88/(g2^2*y) - (g1*t^6.31)/(g2^6*y) - (g2^5*t^6.63)/(g1*y) - t^6.76/(g2^4*y) - t^7.21/(g1*g2^2*y) - (g1*t^7.25)/(g2^7*y) - (g2^4*t^7.57)/(g1*y) - (g1*t^7.61)/(g2*y) - t^7.7/(g2^5*y) + (g2*t^8.06)/y - t^8.15/(g1*g2^3*y) + (g1*t^8.19)/(g2^8*y) - (2*g1*t^8.55)/(g2^2*y) + t^8.64/(g2^6*y) - (g1^2*t^8.68)/(g2^11*y) + (g2^5*t^8.96)/(g1^2*y) - (t^3.94*y)/g2 - (t^4.88*y)/g2^2 - (g1*t^6.31*y)/g2^6 - (g2^5*t^6.63*y)/g1 - (t^6.76*y)/g2^4 - (t^7.21*y)/(g1*g2^2) - (g1*t^7.25*y)/g2^7 - (g2^4*t^7.57*y)/g1 - (g1*t^7.61*y)/g2 - (t^7.7*y)/g2^5 + g2*t^8.06*y - (t^8.15*y)/(g1*g2^3) + (g1*t^8.19*y)/g2^8 - (2*g1*t^8.55*y)/g2^2 + (t^8.64*y)/g2^6 - (g1^2*t^8.68*y)/g2^11 + (g2^5*t^8.96*y)/g1^2 + (t^8.82*y^2)/g2^3 |
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 |
---|---|---|---|---|---|---|---|---|---|
57691 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ | 1.4007 | 1.5922 | 0.8798 | [X:[1.3576], M:[0.791], q:[0.6667, 0.3455], qb:[0.5424, 0.5184], phi:[0.3212]] | t^2.37 + t^2.59 + t^2.66 + t^2.89 + 2*t^3.56 + t^3.63 + t^4.07 + 2*t^4.52 + 2*t^4.59 + t^4.75 + t^4.96 + t^5.04 + t^5.18 + 2*t^5.26 + t^5.33 + 2*t^5.48 + 2*t^5.55 + t^5.7 + t^5.77 + t^5.78 + t^5.93 - t^6. - t^3.96/y - t^4.93/y - t^3.96*y - t^4.93*y | detail |