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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46089 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$ + ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{1}$ | 0.561 | 0.7216 | 0.7774 | [M:[0.7295, 1.1401, 0.7101], q:[0.2802, 0.9903], qb:[0.5797, 0.43], phi:[0.43]] | [M:[[11], [-2], [-3]], q:[[-4], [-7]], qb:[[6], [1]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{3}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}^{3}q_{1}^{2}$, ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{4}$ | ${}\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ | -1 | 2*t^2.13 + t^2.189 + t^2.58 + t^2.971 + t^3.029 + 2*t^3.42 + 4*t^4.261 + 2*t^4.319 + t^4.377 + 3*t^4.71 + t^4.768 + 2*t^5.101 + 3*t^5.159 + t^5.218 + 4*t^5.551 + 2*t^5.609 + t^5.942 - t^6. + t^6.058 + 6*t^6.391 + 3*t^6.449 + 2*t^6.508 + t^6.566 + 4*t^6.841 + 2*t^6.899 + t^6.957 + 3*t^7.232 + 3*t^7.29 + 3*t^7.348 + t^7.406 + 6*t^7.681 + 3*t^7.739 + 2*t^7.797 + 2*t^8.072 - 3*t^8.13 + t^8.247 + 8*t^8.522 + t^8.58 + 3*t^8.638 + 2*t^8.696 + t^8.754 + t^8.913 + 2*t^8.971 - t^4.29/y - t^6.42/y - t^6.478/y + t^7.261/y + (2*t^7.319)/y + (2*t^7.71)/y + t^7.768/y + (3*t^8.101)/y + (4*t^8.159)/y + t^8.218/y + (4*t^8.551)/y + (2*t^8.609)/y - t^8.667/y - t^4.29*y - t^6.42*y - t^6.478*y + t^7.261*y + 2*t^7.319*y + 2*t^7.71*y + t^7.768*y + 3*t^8.101*y + 4*t^8.159*y + t^8.218*y + 4*t^8.551*y + 2*t^8.609*y - t^8.667*y | (2*t^2.13)/g1^3 + g1^11*t^2.189 + g1^2*t^2.58 + t^2.971/g1^7 + g1^7*t^3.029 + (2*t^3.42)/g1^2 + (4*t^4.261)/g1^6 + 2*g1^8*t^4.319 + g1^22*t^4.377 + (3*t^4.71)/g1 + g1^13*t^4.768 + (2*t^5.101)/g1^10 + 3*g1^4*t^5.159 + g1^18*t^5.218 + (4*t^5.551)/g1^5 + 2*g1^9*t^5.609 + t^5.942/g1^14 - t^6. + g1^14*t^6.058 + (6*t^6.391)/g1^9 + 3*g1^5*t^6.449 + 2*g1^19*t^6.508 + g1^33*t^6.566 + (4*t^6.841)/g1^4 + 2*g1^10*t^6.899 + g1^24*t^6.957 + (3*t^7.232)/g1^13 + 3*g1*t^7.29 + 3*g1^15*t^7.348 + g1^29*t^7.406 + (6*t^7.681)/g1^8 + 3*g1^6*t^7.739 + 2*g1^20*t^7.797 + (2*t^8.072)/g1^17 - (3*t^8.13)/g1^3 + g1^25*t^8.247 + (8*t^8.522)/g1^12 + g1^2*t^8.58 + 3*g1^16*t^8.638 + 2*g1^30*t^8.696 + g1^44*t^8.754 + t^8.913/g1^21 + (2*t^8.971)/g1^7 - (g1*t^4.29)/y - t^6.42/(g1^2*y) - (g1^12*t^6.478)/y + t^7.261/(g1^6*y) + (2*g1^8*t^7.319)/y + (2*t^7.71)/(g1*y) + (g1^13*t^7.768)/y + (3*t^8.101)/(g1^10*y) + (4*g1^4*t^8.159)/y + (g1^18*t^8.218)/y + (4*t^8.551)/(g1^5*y) + (2*g1^9*t^8.609)/y - (g1^23*t^8.667)/y - g1*t^4.29*y - (t^6.42*y)/g1^2 - g1^12*t^6.478*y + (t^7.261*y)/g1^6 + 2*g1^8*t^7.319*y + (2*t^7.71*y)/g1 + g1^13*t^7.768*y + (3*t^8.101*y)/g1^10 + 4*g1^4*t^8.159*y + g1^18*t^8.218*y + (4*t^8.551*y)/g1^5 + 2*g1^9*t^8.609*y - g1^23*t^8.667*y |
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 |
---|---|---|---|---|---|---|---|---|---|
46061 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$ | 0.5407 | 0.6833 | 0.7913 | [M:[0.7245, 1.141], q:[0.282, 0.9935], qb:[0.577, 0.4295], phi:[0.4295]] | t^2.134 + t^2.174 + t^2.577 + t^2.98 + t^3.02 + 2*t^3.423 + t^3.866 + 2*t^4.269 + t^4.308 + t^4.347 + 2*t^4.711 + t^4.751 + t^5.115 + 2*t^5.154 + t^5.193 + 2*t^5.557 + 2*t^5.597 + t^5.961 - t^4.289/y - t^4.289*y | detail |