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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58094 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ | 1.4419 | 1.6274 | 0.886 | [X:[1.344], M:[0.968], q:[0.568, 0.536], qb:[0.432, 0.4959], phi:[0.328]] | [X:[[6]], M:[[-18]], q:[[7], [-11]], qb:[[-7], [29]], phi:[[-3]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$ | ${}$ | -2 | 2*t^2.9 + t^2.95 + t^3. + t^3.19 + t^3.89 + t^3.98 + t^4.03 + t^4.08 + t^4.18 + t^4.87 + t^4.97 + 2*t^5.06 + t^5.16 + t^5.26 + 2*t^5.81 + 2*t^5.86 + 3*t^5.9 + t^5.95 - 2*t^6. + t^6.05 + t^6.1 + t^6.14 + t^6.24 + t^6.38 + t^6.79 + 2*t^6.84 + 3*t^6.89 + 3*t^6.94 + 2*t^6.98 + 3*t^7.03 + 2*t^7.08 + t^7.13 + 2*t^7.22 + t^7.27 + t^7.37 + t^7.42 + 3*t^7.78 + 3*t^7.87 + t^7.92 + 5*t^7.97 + t^8.02 + 5*t^8.06 + t^8.11 + 3*t^8.16 + t^8.21 + 3*t^8.26 + t^8.35 + t^8.45 + t^8.71 + 3*t^8.76 + 3*t^8.81 + 4*t^8.86 - 4*t^8.9 + 4*t^8.95 + t^8.95/y^2 - t^3.98/y - t^4.97/y - (2*t^6.89)/y - t^6.94/y - t^6.98/y - t^7.18/y - (2*t^7.87)/y - t^7.92/y - t^7.97/y - t^8.16/y + t^8.81/y + t^8.86/y + (2*t^8.9)/y - t^3.98*y - t^4.97*y - 2*t^6.89*y - t^6.94*y - t^6.98*y - t^7.18*y - 2*t^7.87*y - t^7.92*y - t^7.97*y - t^8.16*y + t^8.81*y + t^8.86*y + 2*t^8.9*y + t^8.95*y^2 | (2*t^2.9)/g1^18 + t^2.95/g1^9 + t^3. + g1^36*t^3.19 + t^3.89/g1^21 + t^3.98/g1^3 + g1^6*t^4.03 + g1^15*t^4.08 + g1^33*t^4.18 + t^4.87/g1^24 + t^4.97/g1^6 + 2*g1^12*t^5.06 + g1^30*t^5.16 + g1^48*t^5.26 + (2*t^5.81)/g1^36 + (2*t^5.86)/g1^27 + (3*t^5.9)/g1^18 + t^5.95/g1^9 - 2*t^6. + g1^9*t^6.05 + g1^18*t^6.1 + g1^27*t^6.14 + g1^45*t^6.24 + g1^72*t^6.38 + t^6.79/g1^39 + (2*t^6.84)/g1^30 + (3*t^6.89)/g1^21 + (3*t^6.94)/g1^12 + (2*t^6.98)/g1^3 + 3*g1^6*t^7.03 + 2*g1^15*t^7.08 + g1^24*t^7.13 + 2*g1^42*t^7.22 + g1^51*t^7.27 + g1^69*t^7.37 + g1^78*t^7.42 + (3*t^7.78)/g1^42 + (3*t^7.87)/g1^24 + t^7.92/g1^15 + (5*t^7.97)/g1^6 + g1^3*t^8.02 + 5*g1^12*t^8.06 + g1^21*t^8.11 + 3*g1^30*t^8.16 + g1^39*t^8.21 + 3*g1^48*t^8.26 + g1^66*t^8.35 + g1^84*t^8.45 + t^8.71/g1^54 + (3*t^8.76)/g1^45 + (3*t^8.81)/g1^36 + (4*t^8.86)/g1^27 - (4*t^8.9)/g1^18 + (4*t^8.95)/g1^9 + t^8.95/(g1^9*y^2) - t^3.98/(g1^3*y) - t^4.97/(g1^6*y) - (2*t^6.89)/(g1^21*y) - t^6.94/(g1^12*y) - t^6.98/(g1^3*y) - (g1^33*t^7.18)/y - (2*t^7.87)/(g1^24*y) - t^7.92/(g1^15*y) - t^7.97/(g1^6*y) - (g1^30*t^8.16)/y + t^8.81/(g1^36*y) + t^8.86/(g1^27*y) + (2*t^8.9)/(g1^18*y) - (t^3.98*y)/g1^3 - (t^4.97*y)/g1^6 - (2*t^6.89*y)/g1^21 - (t^6.94*y)/g1^12 - (t^6.98*y)/g1^3 - g1^33*t^7.18*y - (2*t^7.87*y)/g1^24 - (t^7.92*y)/g1^15 - (t^7.97*y)/g1^6 - g1^30*t^8.16*y + (t^8.81*y)/g1^36 + (t^8.86*y)/g1^27 + (2*t^8.9*y)/g1^18 + (t^8.95*y^2)/g1^9 |
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 |
---|---|---|---|---|---|---|---|---|---|
57333 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ | 1.4535 | 1.6404 | 0.8861 | [X:[1.3366], M:[0.9901], q:[0.5074, 0.4975], qb:[0.4926, 0.5124], phi:[0.3317]] | 2*t^2.97 + t^2.985 + t^3. + t^3.059 + t^3.965 + t^3.995 + t^4.01 + t^4.025 + t^4.054 + t^4.96 + t^4.99 + t^5.02 + t^5.049 + t^5.488 + t^5.502 + t^5.532 + t^5.547 + 2*t^5.941 + 2*t^5.955 + 2*t^5.97 + t^5.985 - 3*t^6. - t^3.995/y - t^4.99/y - t^3.995*y - t^4.99*y | detail |