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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57771 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ | 1.4577 | 1.6475 | 0.8848 | [X:[1.3452], M:[0.9288, 0.9644], q:[0.4738, 0.545], qb:[0.4906, 0.5262], phi:[0.3274]] | [X:[[0, 2]], M:[[0, -12], [0, -6]], q:[[-1, 0], [-1, 12]], qb:[[1, -6], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{6}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | ${}$ | -3 | t^2.79 + 2*t^2.89 + t^2.95 + t^3. + t^3.88 + t^3.98 + t^4.04 + t^4.09 + t^4.2 + t^4.86 + t^4.96 + t^5.07 + t^5.18 + t^5.46 + t^5.5 + t^5.57 + t^5.61 + t^5.67 + 2*t^5.68 + t^5.73 + 3*t^5.79 + 2*t^5.84 + 2*t^5.89 + t^5.95 - 3*t^6. - t^6.11 - t^6.21 + t^6.44 + t^6.49 + t^6.59 + 2*t^6.66 + 2*t^6.77 + 2*t^6.82 + 3*t^6.88 + 3*t^6.93 + 2*t^6.98 + 2*t^7.04 + 2*t^7.09 + t^7.14 + t^7.21 + t^7.36 + t^7.47 - t^7.48 - t^7.63 + 2*t^7.64 + t^7.68 + 3*t^7.75 + t^7.8 + t^7.85 + 4*t^7.86 + t^7.91 + 4*t^7.96 + t^8.02 + 4*t^8.07 + t^8.12 + 2*t^8.18 + t^8.28 + t^8.35 + t^8.36 + t^8.39 + t^8.4 + t^8.41 + t^8.45 + 2*t^8.47 + t^8.5 + t^8.52 + t^8.56 + 3*t^8.57 - t^8.61 + t^8.62 + 2*t^8.63 + 4*t^8.68 - t^8.72 + 4*t^8.73 - t^8.78 + 4*t^8.84 - 6*t^8.89 + t^8.95 + t^8.95/y^2 - t^3.98/y - t^4.96/y - t^6.77/y - (2*t^6.88)/y - t^6.93/y - t^6.98/y - t^7.75/y - (2*t^7.86)/y - t^7.91/y - t^7.96/y + (2*t^8.68)/y + t^8.73/y + (2*t^8.79)/y + t^8.84/y + (2*t^8.89)/y - t^3.98*y - t^4.96*y - t^6.77*y - 2*t^6.88*y - t^6.93*y - t^6.98*y - t^7.75*y - 2*t^7.86*y - t^7.91*y - t^7.96*y + 2*t^8.68*y + t^8.73*y + 2*t^8.79*y + t^8.84*y + 2*t^8.89*y + t^8.95*y^2 | t^2.79/g2^12 + (2*t^2.89)/g2^6 + t^2.95/g2^3 + t^3. + t^3.88/g2^7 + t^3.98/g2 + g2^2*t^4.04 + g2^5*t^4.09 + g2^11*t^4.2 + t^4.86/g2^8 + t^4.96/g2^2 + g2^4*t^5.07 + g2^10*t^5.18 + (g2^11*t^5.46)/g1^3 + (g1^3*t^5.5)/g2^13 + t^5.57/g2^24 + (g1^3*t^5.61)/g2^7 + (g2^23*t^5.67)/g1^3 + (2*t^5.68)/g2^18 + t^5.73/g2^15 + (3*t^5.79)/g2^12 + (2*t^5.84)/g2^9 + (2*t^5.89)/g2^6 + t^5.95/g2^3 - 3*t^6. - g2^6*t^6.11 - g2^12*t^6.21 + (g2^10*t^6.44)/g1^3 + (g1^3*t^6.49)/g2^14 + (g1^3*t^6.59)/g2^8 + t^6.66/g2^19 + (g2^22*t^6.66)/g1^3 + (2*t^6.77)/g2^13 + (2*t^6.82)/g2^10 + (3*t^6.88)/g2^7 + (3*t^6.93)/g2^4 + (2*t^6.98)/g2 + 2*g2^2*t^7.04 + 2*g2^5*t^7.09 + g2^8*t^7.14 + t^7.21/(g1^3*g2^3) + (g1^3*t^7.36)/g2^21 - (g1^3*t^7.42)/g2^18 + (g2^9*t^7.42)/g1^3 + (g1^3*t^7.47)/g2^15 - (g2^12*t^7.48)/g1^3 + (g1^3*t^7.58)/g2^9 - (g2^18*t^7.58)/g1^3 - (g1^3*t^7.63)/g2^6 + t^7.64/g2^20 + (g2^21*t^7.64)/g1^3 + (g1^3*t^7.68)/g2^3 + (3*t^7.75)/g2^14 + t^7.8/g2^11 + (g2^33*t^7.85)/g1^3 + (4*t^7.86)/g2^8 + t^7.91/g2^5 + (4*t^7.96)/g2^2 + g2*t^8.02 + 4*g2^4*t^8.07 + g2^7*t^8.12 + 2*g2^10*t^8.18 + g2^16*t^8.28 + (g2^5*t^8.35)/g1^3 + t^8.36/g2^36 + g2^22*t^8.39 + (g1^3*t^8.4)/g2^19 + (g2^8*t^8.41)/g1^3 + (g1^3*t^8.45)/g2^16 + (2*t^8.47)/g2^30 + (g1^3*t^8.5)/g2^13 + t^8.52/g2^27 + (g1^3*t^8.56)/g2^10 + (3*t^8.57)/g2^24 - (g1^3*t^8.61)/g2^7 + (g2^20*t^8.62)/g1^3 + (2*t^8.63)/g2^21 + (4*t^8.68)/g2^18 - (g1^3*t^8.72)/g2 + (4*t^8.73)/g2^15 - (g2^29*t^8.78)/g1^3 + (4*t^8.84)/g2^9 - (6*t^8.89)/g2^6 + t^8.95/g2^3 + t^8.95/(g2^3*y^2) - t^3.98/(g2*y) - t^4.96/(g2^2*y) - t^6.77/(g2^13*y) - (2*t^6.88)/(g2^7*y) - t^6.93/(g2^4*y) - t^6.98/(g2*y) - t^7.75/(g2^14*y) - (2*t^7.86)/(g2^8*y) - t^7.91/(g2^5*y) - t^7.96/(g2^2*y) + (2*t^8.68)/(g2^18*y) + t^8.73/(g2^15*y) + (2*t^8.79)/(g2^12*y) + t^8.84/(g2^9*y) + (2*t^8.89)/(g2^6*y) - (t^3.98*y)/g2 - (t^4.96*y)/g2^2 - (t^6.77*y)/g2^13 - (2*t^6.88*y)/g2^7 - (t^6.93*y)/g2^4 - (t^6.98*y)/g2 - (t^7.75*y)/g2^14 - (2*t^7.86*y)/g2^8 - (t^7.91*y)/g2^5 - (t^7.96*y)/g2^2 + (2*t^8.68*y)/g2^18 + (t^8.73*y)/g2^15 + (2*t^8.79*y)/g2^12 + (t^8.84*y)/g2^9 + (2*t^8.89*y)/g2^6 + (t^8.95*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 |
---|---|---|---|---|---|---|---|---|---|
57284 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ | 1.4577 | 1.6478 | 0.8847 | [X:[1.3444], M:[0.9302, 0.9634], q:[0.4722, 0.5455], qb:[0.4912, 0.5243], phi:[0.3278]] | t^2.791 + 2*t^2.89 + t^2.95 + t^2.989 + t^3.873 + t^3.973 + t^4.033 + t^4.093 + t^4.193 + t^4.857 + t^4.956 + t^5.077 + t^5.176 + t^5.453 + t^5.503 + t^5.581 + t^5.603 + t^5.673 + 2*t^5.681 + t^5.741 + 3*t^5.78 + 2*t^5.84 + 2*t^5.879 + t^5.94 + t^5.979 - 4*t^6. - t^3.983/y - t^4.967/y - t^3.983*y - t^4.967*y | detail |