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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60767 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ | 1.3666 | 1.5946 | 0.857 | [X:[1.3509], M:[0.7547, 0.7547], q:[0.3435, 0.5887], qb:[0.6565, 0.3056], phi:[0.3509]] | [X:[[0, 1]], M:[[0, 5], [0, 5]], q:[[-1, -1], [-1, -6]], qb:[[1, 1], [1, 0]], phi:[[0, 1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}^{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{5}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$ | ${}\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$ | -2 | t^2.11 + 2*t^2.26 + t^2.68 + 2*t^3. + t^3.16 + 3*t^4.05 + t^4.21 + 2*t^4.37 + 3*t^4.53 + 3*t^4.79 + t^4.86 + t^4.88 + t^4.95 + 3*t^5.11 + 4*t^5.26 + t^5.37 + 2*t^5.42 + t^5.62 + 2*t^5.68 + 2*t^5.84 + 3*t^5.91 + t^5.93 - 2*t^6. + 5*t^6.16 + t^6.25 + 7*t^6.32 + 2*t^6.48 + 3*t^6.63 + t^6.67 + 2*t^6.74 + 4*t^6.79 - t^6.83 + 2*t^6.89 + 3*t^6.96 + 2*t^6.99 + 6*t^7.05 + t^7.14 + 7*t^7.21 + 5*t^7.37 + 3*t^7.47 + 6*t^7.53 + t^7.54 + t^7.56 + 3*t^7.69 + 2*t^7.72 + 5*t^7.79 + t^7.88 + 3*t^7.95 + 5*t^8.01 + 2*t^8.04 + t^8.05 + 6*t^8.11 + 3*t^8.17 + t^8.26 + t^8.3 + t^8.36 + 2*t^8.37 + 10*t^8.42 + t^8.46 + 2*t^8.51 + 2*t^8.52 + 11*t^8.58 + 3*t^8.59 + t^8.62 - 4*t^8.68 + 3*t^8.74 - 2*t^8.75 + t^8.77 + 10*t^8.84 + 4*t^8.9 + 4*t^8.91 + 2*t^8.93 - t^4.05/y - t^5.11/y - t^6.16/y - (2*t^6.32)/y - t^6.74/y - t^7.05/y - (2*t^7.21)/y + t^7.53/y + t^7.79/y + (3*t^7.95)/y - t^8.11/y + (3*t^8.26)/y - (3*t^8.58)/y + (2*t^8.68)/y - t^4.05*y - t^5.11*y - t^6.16*y - 2*t^6.32*y - t^6.74*y - t^7.05*y - 2*t^7.21*y + t^7.53*y + t^7.79*y + 3*t^7.95*y - t^8.11*y + 3*t^8.26*y - 3*t^8.58*y + 2*t^8.68*y | g2^2*t^2.11 + 2*g2^5*t^2.26 + t^2.68/g2^6 + 2*t^3. + g2^3*t^3.16 + 3*g2*t^4.05 + g2^4*t^4.21 + 2*g2^7*t^4.37 + 3*g2^10*t^4.53 + (3*t^4.79)/g2^4 + g1^3*g2^2*t^4.86 + t^4.88/(g1^3*g2^7) + t^4.95/g2 + 3*g2^2*t^5.11 + 4*g2^5*t^5.26 + t^5.37/g2^12 + 2*g2^8*t^5.42 + t^5.62/(g1^3*g2^12) + (2*t^5.68)/g2^6 + (2*t^5.84)/g2^3 + 3*g1^3*g2^3*t^5.91 + t^5.93/(g1^3*g2^6) - 2*t^6. + 5*g2^3*t^6.16 + t^6.25/g1^3 + 7*g2^6*t^6.32 + 2*g2^9*t^6.48 + 3*g2^12*t^6.63 + t^6.67/(g1^3*g2^11) + (2*t^6.74)/g2^5 + 4*g2^15*t^6.79 - t^6.83/(g1^3*g2^8) + (2*t^6.89)/g2^2 + 3*g1^3*g2^4*t^6.96 + (2*t^6.99)/(g1^3*g2^5) + 6*g2*t^7.05 + t^7.14/(g1^3*g2^2) + 7*g2^4*t^7.21 + 5*g2^7*t^7.37 + (3*t^7.47)/g2^10 + 6*g2^10*t^7.53 + (g1^3*t^7.54)/g2^4 + t^7.56/(g1^3*g2^13) + 3*g2^13*t^7.69 + (2*t^7.72)/(g1^3*g2^10) + (5*t^7.79)/g2^4 + t^7.88/(g1^3*g2^7) + (3*t^7.95)/g2 + 5*g1^3*g2^5*t^8.01 + (2*t^8.04)/(g1^3*g2^4) + t^8.05/g2^18 + 6*g2^2*t^8.11 + 3*g1^3*g2^8*t^8.17 + g2^5*t^8.26 + t^8.3/(g1^3*g2^18) + (g2^2*t^8.36)/g1^3 + (2*t^8.37)/g2^12 + 10*g2^8*t^8.42 + t^8.46/(g1^3*g2^15) + (2*g2^5*t^8.51)/g1^3 + (2*t^8.52)/g2^9 + 11*g2^11*t^8.58 + (3*g1^3*t^8.59)/g2^3 + t^8.62/(g1^3*g2^12) - (4*t^8.68)/g2^6 + 3*g2^14*t^8.74 - 2*g1^3*t^8.75 + t^8.77/(g1^3*g2^9) + (10*t^8.84)/g2^3 + 4*g2^17*t^8.9 + 4*g1^3*g2^3*t^8.91 + (2*t^8.93)/(g1^3*g2^6) - (g2*t^4.05)/y - (g2^2*t^5.11)/y - (g2^3*t^6.16)/y - (2*g2^6*t^6.32)/y - t^6.74/(g2^5*y) - (g2*t^7.05)/y - (2*g2^4*t^7.21)/y + (g2^10*t^7.53)/y + t^7.79/(g2^4*y) + (3*t^7.95)/(g2*y) - (g2^2*t^8.11)/y + (3*g2^5*t^8.26)/y - (3*g2^11*t^8.58)/y + (2*t^8.68)/(g2^6*y) - g2*t^4.05*y - g2^2*t^5.11*y - g2^3*t^6.16*y - 2*g2^6*t^6.32*y - (t^6.74*y)/g2^5 - g2*t^7.05*y - 2*g2^4*t^7.21*y + g2^10*t^7.53*y + (t^7.79*y)/g2^4 + (3*t^7.95*y)/g2 - g2^2*t^8.11*y + 3*g2^5*t^8.26*y - 3*g2^11*t^8.58*y + (2*t^8.68*y)/g2^6 |
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 |
---|---|---|---|---|---|---|---|---|---|
57470 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ | 1.348 | 1.5616 | 0.8633 | [X:[1.354], M:[0.7701], q:[0.3455, 0.5754], qb:[0.6545, 0.3005], phi:[0.354]] | t^2.12 + t^2.31 + t^2.63 + 2*t^3. + t^3.19 + t^3.69 + 3*t^4.06 + t^4.25 + t^4.43 + t^4.62 + 3*t^4.75 + t^4.83 + t^4.86 + 3*t^5.12 + t^5.26 + 2*t^5.31 + t^5.5 + t^5.55 + 2*t^5.63 + 3*t^5.81 + 3*t^5.89 + t^5.92 - t^6. - t^4.06/y - t^5.12/y - t^4.06*y - t^5.12*y | detail |