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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58621 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }q_{1}\tilde{q}_{2}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ | 0.8147 | 0.8805 | 0.9253 | [X:[1.5438, 1.3687], M:[1.3157], q:[0.6843, 0.4032], qb:[0.2281, 1.3157], phi:[0.2281]] | [X:[[-2], [6]], M:[[-3]], q:[[3], [-7]], qb:[[1], [-3]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }X_{2}$, ${ }X_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$ | ${}$ | -2 | t^2.58 + t^3.26 + t^3.95 + 2*t^4.11 + t^4.63 + t^5.16 + t^5.68 + t^5.84 - 2*t^6. + 2*t^6.53 + t^6.68 - t^6.84 + t^7.21 + 2*t^7.37 - t^7.53 + t^7.73 + t^7.89 + 2*t^8.05 + 2*t^8.21 + t^8.26 - 2*t^8.58 + 2*t^8.74 + t^8.94 + t^8.05/y^2 - t^3.68/y - t^4.37/y - t^6.95/y - t^7.63/y - t^7.79/y - t^8.32/y - t^8.47/y + t^8.84/y - t^3.68*y - t^4.37*y - t^6.95*y - t^7.63*y - t^7.79*y - t^8.32*y - t^8.47*y + t^8.84*y + t^8.05*y^2 | t^2.58/g1^5 + t^3.26/g1^4 + t^3.95/g1^3 + 2*g1^6*t^4.11 + t^4.63/g1^2 + t^5.16/g1^10 + t^5.68/g1^18 + t^5.84/g1^9 - 2*t^6. + (2*t^6.53)/g1^8 + g1*t^6.68 - g1^10*t^6.84 + t^7.21/g1^7 + 2*g1^2*t^7.37 - g1^11*t^7.53 + t^7.73/g1^15 + t^7.89/g1^6 + 2*g1^3*t^8.05 + 2*g1^12*t^8.21 + t^8.26/g1^23 - (2*t^8.58)/g1^5 + 2*g1^4*t^8.74 + t^8.94/g1^22 + (g1^3*t^8.05)/y^2 - (g1*t^3.68)/y - (g1^2*t^4.37)/y - t^6.95/(g1^3*y) - t^7.63/(g1^2*y) - (g1^7*t^7.79)/y - t^8.32/(g1*y) - (g1^8*t^8.47)/y + t^8.84/(g1^9*y) - g1*t^3.68*y - g1^2*t^4.37*y - (t^6.95*y)/g1^3 - (t^7.63*y)/g1^2 - g1^7*t^7.79*y - (t^8.32*y)/g1 - g1^8*t^8.47*y + (t^8.84*y)/g1^9 + g1^3*t^8.05*y^2 |
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 |
---|---|---|---|---|---|---|---|---|---|
57653 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.4123 | 1.5667 | 0.9014 | [X:[1.4039], M:[1.1059], q:[0.5961, 0.5099], qb:[0.5961, 0.5099], phi:[0.298]] | t^3.06 + 3*t^3.32 + t^3.58 + t^3.95 + 3*t^4.21 + t^4.47 + t^4.85 + 2*t^5.11 + t^5.36 - 2*t^6. - t^3.89/y - t^4.79/y - t^3.89*y - t^4.79*y | detail |