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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58358 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$ | 1.4112 | 1.6637 | 0.8482 | [X:[], M:[0.7819, 1.1785], q:[0.3989, 0.4023], qb:[0.4192, 0.3796], phi:[0.4]] | [X:[], M:[[-2, -1], [1, 2]], q:[[1, 1], [-2, -2]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${2}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ | 0 | t^2.34 + 2*t^2.35 + t^2.4 + t^2.45 + 2*t^3.54 + t^3.55 + t^3.6 + t^3.66 + t^4.67 + 2*t^4.68 + 3*t^4.69 + 3*t^4.74 + 3*t^4.75 + t^4.79 + 4*t^4.8 + t^4.81 + 3*t^4.85 + t^4.86 + t^4.91 + 2*t^5.87 + 4*t^5.88 + 2*t^5.89 + 4*t^5.94 + 3*t^5.95 + t^5.99 + 2*t^6.01 + 2*t^6.05 + t^6.06 + t^7.01 + 3*t^7.02 + 3*t^7.03 + 4*t^7.04 + 6*t^7.07 + 8*t^7.08 + 6*t^7.09 + t^7.13 + 8*t^7.14 + 8*t^7.15 + 2*t^7.16 + 4*t^7.19 + 9*t^7.2 + 4*t^7.21 + t^7.22 + t^7.24 + 6*t^7.25 + t^7.26 + 3*t^7.31 + t^7.33 + t^7.36 + t^7.37 + 2*t^8.21 + 4*t^8.22 + 6*t^8.23 + 3*t^8.24 + 7*t^8.27 + 10*t^8.28 + 6*t^8.29 + t^8.33 + 5*t^8.34 + t^8.35 + 3*t^8.36 + 4*t^8.39 + 4*t^8.4 + 3*t^8.41 + t^8.44 - t^8.45 - t^8.46 + t^8.51 + t^8.53 - t^4.2/y - t^5.4/y - t^6.54/y - (2*t^6.55)/y - t^6.6/y - t^6.65/y + (2*t^7.68)/y + t^7.69/y - t^7.74/y + t^7.79/y + t^7.8/y + t^7.85/y + t^8.87/y + (3*t^8.88)/y - t^8.89/y + t^8.99/y - t^4.2*y - t^5.4*y - t^6.54*y - 2*t^6.55*y - t^6.6*y - t^6.65*y + 2*t^7.68*y + t^7.69*y - t^7.74*y + t^7.79*y + t^7.8*y + t^7.85*y + t^8.87*y + 3*t^8.88*y - t^8.89*y + t^8.99*y | g1*g2^2*t^2.34 + (2*t^2.35)/(g1^2*g2) + t^2.4 + g1^2*g2*t^2.45 + 2*g1*g2^2*t^3.54 + t^3.55/(g1^2*g2) + t^3.6 + t^3.66/(g1*g2^2) + g1^2*g2^4*t^4.67 + (2*g2*t^4.68)/g1 + (3*t^4.69)/(g1^4*g2^2) + 3*g1*g2^2*t^4.74 + (3*t^4.75)/(g1^2*g2) + g1^3*g2^3*t^4.79 + 4*t^4.8 + t^4.81/(g1^3*g2^3) + 3*g1^2*g2*t^4.85 + t^4.86/(g1*g2^2) + g1^4*g2^2*t^4.91 + 2*g1^2*g2^4*t^5.87 + (4*g2*t^5.88)/g1 + (2*t^5.89)/(g1^4*g2^2) + 4*g1*g2^2*t^5.94 + (3*t^5.95)/(g1^2*g2) + g1^3*g2^3*t^5.99 + (2*t^6.01)/(g1^3*g2^3) + 2*g1^2*g2*t^6.05 + t^6.06/(g1*g2^2) + g1^3*g2^6*t^7.01 + 3*g2^3*t^7.02 + (3*t^7.03)/g1^3 + (4*t^7.04)/(g1^6*g2^3) + 6*g1^2*g2^4*t^7.07 + (8*g2*t^7.08)/g1 + (6*t^7.09)/(g1^4*g2^2) + g1^4*g2^5*t^7.13 + 8*g1*g2^2*t^7.14 + (8*t^7.15)/(g1^2*g2) + (2*t^7.16)/(g1^5*g2^4) + 4*g1^3*g2^3*t^7.19 + 9*t^7.2 + (4*t^7.21)/(g1^3*g2^3) + t^7.22/(g1^6*g2^6) + g1^5*g2^4*t^7.24 + 6*g1^2*g2*t^7.25 + t^7.26/(g1*g2^2) + 3*g1^4*g2^2*t^7.31 + t^7.33/(g1^2*g2^4) + g1^6*g2^3*t^7.36 + g1^3*t^7.37 + 2*g1^3*g2^6*t^8.21 + 4*g2^3*t^8.22 + (6*t^8.23)/g1^3 + (3*t^8.24)/(g1^6*g2^3) + 7*g1^2*g2^4*t^8.27 + (10*g2*t^8.28)/g1 + (6*t^8.29)/(g1^4*g2^2) + g1^4*g2^5*t^8.33 + 5*g1*g2^2*t^8.34 + t^8.35/(g1^2*g2) + (3*t^8.36)/(g1^5*g2^4) + 4*g1^3*g2^3*t^8.39 + 4*t^8.4 + (3*t^8.41)/(g1^3*g2^3) + g1^5*g2^4*t^8.44 - g1^2*g2*t^8.45 - t^8.46/(g1*g2^2) + g1^4*g2^2*t^8.51 + t^8.53/(g1^2*g2^4) - t^4.2/y - t^5.4/y - (g1*g2^2*t^6.54)/y - (2*t^6.55)/(g1^2*g2*y) - t^6.6/y - (g1^2*g2*t^6.65)/y + (2*g2*t^7.68)/(g1*y) + t^7.69/(g1^4*g2^2*y) - (g1*g2^2*t^7.74)/y + (g1^3*g2^3*t^7.79)/y + t^7.8/y + (g1^2*g2*t^7.85)/y + (g1^2*g2^4*t^8.87)/y + (3*g2*t^8.88)/(g1*y) - t^8.89/(g1^4*g2^2*y) + (g1^3*g2^3*t^8.99)/y - t^4.2*y - t^5.4*y - g1*g2^2*t^6.54*y - (2*t^6.55*y)/(g1^2*g2) - t^6.6*y - g1^2*g2*t^6.65*y + (2*g2*t^7.68*y)/g1 + (t^7.69*y)/(g1^4*g2^2) - g1*g2^2*t^7.74*y + g1^3*g2^3*t^7.79*y + t^7.8*y + g1^2*g2*t^7.85*y + g1^2*g2^4*t^8.87*y + (3*g2*t^8.88*y)/g1 - (t^8.89*y)/(g1^4*g2^2) + g1^3*g2^3*t^8.99*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 |
---|---|---|---|---|---|---|---|---|---|
57353 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ | 1.4112 | 1.6637 | 0.8482 | [M:[0.7823, 1.1779], q:[0.3977, 0.402], qb:[0.4201, 0.3803], phi:[0.4]] | t^2.334 + 2*t^2.347 + t^2.4 + t^2.453 + 2*t^3.534 + t^3.547 + t^3.6 + t^3.666 + t^4.668 + 2*t^4.681 + 3*t^4.694 + 2*t^4.734 + t^4.742 + 3*t^4.747 + t^4.787 + t^4.792 + 3*t^4.8 + t^4.805 + 2*t^4.853 + t^4.861 + t^4.866 + t^4.906 + 2*t^5.868 + 4*t^5.881 + 2*t^5.894 + 3*t^5.934 + t^5.942 + 3*t^5.947 + t^5.987 + t^5.992 - t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail |