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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57910 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}^{2}$ + ${ }q_{1}\tilde{q}_{1}X_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ | 1.3303 | 1.5564 | 0.8547 | [X:[1.2, 1.4], M:[1.0, 0.7819], q:[0.2924, 0.5106], qb:[0.3076, 0.4894], phi:[0.4]] | [X:[[0, 0], [0, 0]], M:[[0, 0], [-1, 1]], q:[[-1, 0], [0, -1]], 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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${}M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }X_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }M_{2}X_{1}$, ${ }q_{1}\tilde{q}_{2}X_{1}$ | ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ | 0 | 2*t^2.35 + t^2.45 + 2*t^3. + t^3.55 + 2*t^3.6 + 3*t^4.2 + t^4.49 + t^4.51 + 3*t^4.69 + t^4.75 + 2*t^4.8 + t^4.85 + t^4.91 + t^5.06 + t^5.14 + 3*t^5.35 + t^5.4 + t^5.45 + t^5.69 + t^5.71 + 2*t^5.89 + 4*t^5.95 + 2*t^6.05 + t^6.23 + t^6.26 + t^6.34 + t^6.37 + 6*t^6.55 + 3*t^6.6 + t^6.65 + 2*t^6.83 + t^6.86 + t^6.89 + t^6.91 + t^6.97 + 4*t^7.04 + 3*t^7.09 + 4*t^7.15 + 8*t^7.2 + t^7.25 + t^7.31 + t^7.36 + 2*t^7.4 + t^7.46 + 2*t^7.49 + t^7.51 + t^7.54 + t^7.6 + 4*t^7.69 + 5*t^7.75 + 5*t^7.8 + t^7.85 + t^7.91 + t^8. + 2*t^8.03 + 2*t^8.06 + t^8.09 + t^8.11 + t^8.2 + 3*t^8.24 + 7*t^8.29 - t^8.35 + 10*t^8.4 - t^8.45 + 2*t^8.51 + 2*t^8.58 + 2*t^8.6 - t^8.63 + t^8.66 + 4*t^8.69 + 3*t^8.71 + t^8.74 - t^8.77 + t^8.82 + 8*t^8.89 + 7*t^8.95 + t^8.97 - t^4.2/y - t^5.4/y - (2*t^6.55)/y - t^6.65/y - t^7.2/y + t^7.69/y - (2*t^7.75)/y + t^7.8/y + (4*t^8.35)/y - (3*t^8.4)/y + (2*t^8.45)/y - t^8.89/y + (3*t^8.95)/y - t^4.2*y - t^5.4*y - 2*t^6.55*y - t^6.65*y - t^7.2*y + t^7.69*y - 2*t^7.75*y + t^7.8*y + 4*t^8.35*y - 3*t^8.4*y + 2*t^8.45*y - t^8.89*y + 3*t^8.95*y | (2*g2*t^2.35)/g1 + (g1*t^2.45)/g2 + 2*t^3. + (g2*t^3.55)/g1 + 2*t^3.6 + 3*t^4.2 + t^4.49/(g1^2*g2) + g1^2*g2*t^4.51 + (3*g2^2*t^4.69)/g1^2 + (g2*t^4.75)/g1 + 2*t^4.8 + (g1*t^4.85)/g2 + (g1^2*t^4.91)/g2^2 + g1*g2^2*t^5.06 + t^5.14/(g1*g2^2) + (3*g2*t^5.35)/g1 + t^5.4 + (g1*t^5.45)/g2 + t^5.69/(g1^2*g2) + g1^2*g2*t^5.71 + (2*g2^2*t^5.89)/g1^2 + (4*g2*t^5.95)/g1 + (2*g1*t^6.05)/g2 + t^6.23/g1^3 + g1*g2^2*t^6.26 + t^6.34/(g1*g2^2) + g1^3*t^6.37 + (6*g2*t^6.55)/g1 + 3*t^6.6 + (g1*t^6.65)/g2 + (2*t^6.83)/g1^3 + g1*g2^2*t^6.86 + t^6.89/(g1^2*g2) + g1^2*g2*t^6.91 + g1^3*t^6.97 + (4*g2^3*t^7.04)/g1^3 + (3*g2^2*t^7.09)/g1^2 + (4*g2*t^7.15)/g1 + 8*t^7.2 + (g1*t^7.25)/g2 + (g1^2*t^7.31)/g2^2 + (g1^3*t^7.36)/g2^3 + 2*g2^3*t^7.4 + g1*g2^2*t^7.46 + (2*t^7.49)/(g1^2*g2) + g1^2*g2*t^7.51 + t^7.54/(g1*g2^2) + t^7.6/g2^3 + (4*g2^2*t^7.69)/g1^2 + (5*g2*t^7.75)/g1 + 5*t^7.8 + (g1*t^7.85)/g2 + (g1^2*t^7.91)/g2^2 + g2^3*t^8. + (2*t^8.03)/g1^3 + 2*g1*g2^2*t^8.06 + t^8.09/(g1^2*g2) + g1^2*g2*t^8.11 + t^8.2/g2^3 + (3*g2^3*t^8.24)/g1^3 + (7*g2^2*t^8.29)/g1^2 - (g2*t^8.35)/g1 + 10*t^8.4 - (g1*t^8.45)/g2 + (2*g1^2*t^8.51)/g2^2 + (2*g2*t^8.58)/g1^4 + 2*g2^3*t^8.6 - t^8.63/g1^3 + g1*g2^2*t^8.66 + (4*t^8.69)/(g1^2*g2) + 3*g1^2*g2*t^8.71 + t^8.74/(g1*g2^2) - g1^3*t^8.77 + (g1^4*t^8.82)/g2 + (8*g2^2*t^8.89)/g1^2 + (7*g2*t^8.95)/g1 + t^8.97/(g1^4*g2^2) - t^4.2/y - t^5.4/y - (2*g2*t^6.55)/(g1*y) - (g1*t^6.65)/(g2*y) - t^7.2/y + (g2^2*t^7.69)/(g1^2*y) - (2*g2*t^7.75)/(g1*y) + t^7.8/y + (4*g2*t^8.35)/(g1*y) - (3*t^8.4)/y + (2*g1*t^8.45)/(g2*y) - (g2^2*t^8.89)/(g1^2*y) + (3*g2*t^8.95)/(g1*y) - t^4.2*y - t^5.4*y - (2*g2*t^6.55*y)/g1 - (g1*t^6.65*y)/g2 - t^7.2*y + (g2^2*t^7.69*y)/g1^2 - (2*g2*t^7.75*y)/g1 + t^7.8*y + (4*g2*t^8.35*y)/g1 - 3*t^8.4*y + (2*g1*t^8.45*y)/g2 - (g2^2*t^8.89*y)/g1^2 + (3*g2*t^8.95*y)/g1 |
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 |
---|---|---|---|---|---|---|---|---|---|
57294 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}^{2}$ + ${ }q_{1}\tilde{q}_{1}X_{2}$ | 1.3133 | 1.5258 | 0.8607 | [X:[1.2, 1.4], M:[1.0], q:[0.3, 0.5], qb:[0.3, 0.5], phi:[0.4]] | 2*t^2.4 + 2*t^3. + 4*t^3.6 + 3*t^4.2 + 2*t^4.5 + 5*t^4.8 + 2*t^5.1 + 3*t^5.4 + 2*t^5.7 + 7*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail | {a: 5253/4000, c: 6103/4000, X1: 6/5, X2: 7/5, M1: 1, q1: 3/10, q2: 1/2, qb1: 3/10, qb2: 1/2, phi1: 2/5} |