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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1852 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ | 0.561 | 0.7216 | 0.7774 | [M:[0.9903, 1.0097, 0.7101, 1.1401, 0.7295], q:[0.5797, 0.9903], qb:[0.43, 0.2802], phi:[0.43]] | [M:[[7], [-7], [3], [2], [-11]], q:[[-6], [7]], qb:[[-1], [4]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }M_{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{5}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{4}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$ | ${}M_{4}q_{1}\tilde{q}_{2}$ | -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*g1^3*t^2.13 + t^2.189/g1^11 + t^2.58/g1^2 + g1^7*t^2.971 + t^3.029/g1^7 + 2*g1^2*t^3.42 + 4*g1^6*t^4.261 + (2*t^4.319)/g1^8 + t^4.377/g1^22 + 3*g1*t^4.71 + t^4.768/g1^13 + 2*g1^10*t^5.101 + (3*t^5.159)/g1^4 + t^5.218/g1^18 + 4*g1^5*t^5.551 + (2*t^5.609)/g1^9 + g1^14*t^5.942 - t^6. + t^6.058/g1^14 + 6*g1^9*t^6.391 + (3*t^6.449)/g1^5 + (2*t^6.508)/g1^19 + t^6.566/g1^33 + 4*g1^4*t^6.841 + (2*t^6.899)/g1^10 + t^6.957/g1^24 + 3*g1^13*t^7.232 + (3*t^7.29)/g1 + (3*t^7.348)/g1^15 + t^7.406/g1^29 + 6*g1^8*t^7.681 + (3*t^7.739)/g1^6 + (2*t^7.797)/g1^20 + 2*g1^17*t^8.072 - 3*g1^3*t^8.13 + t^8.247/g1^25 + 8*g1^12*t^8.522 + t^8.58/g1^2 + (3*t^8.638)/g1^16 + (2*t^8.696)/g1^30 + t^8.754/g1^44 + g1^21*t^8.913 + 2*g1^7*t^8.971 - t^4.29/(g1*y) - (g1^2*t^6.42)/y - t^6.478/(g1^12*y) + (g1^6*t^7.261)/y + (2*t^7.319)/(g1^8*y) + (2*g1*t^7.71)/y + t^7.768/(g1^13*y) + (3*g1^10*t^8.101)/y + (4*t^8.159)/(g1^4*y) + t^8.218/(g1^18*y) + (4*g1^5*t^8.551)/y + (2*t^8.609)/(g1^9*y) - t^8.667/(g1^23*y) - (t^4.29*y)/g1 - g1^2*t^6.42*y - (t^6.478*y)/g1^12 + g1^6*t^7.261*y + (2*t^7.319*y)/g1^8 + 2*g1*t^7.71*y + (t^7.768*y)/g1^13 + 3*g1^10*t^8.101*y + (4*t^8.159*y)/g1^4 + (t^8.218*y)/g1^18 + 4*g1^5*t^8.551*y + (2*t^8.609*y)/g1^9 - (t^8.667*y)/g1^23 |
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 |
---|---|---|---|---|---|---|---|---|---|
463 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}\phi_{1}^{2}$ | 0.5418 | 0.6877 | 0.7879 | [M:[0.9659, 1.0341, 0.6997, 1.1331], q:[0.6007, 0.9659], qb:[0.4334, 0.2662], phi:[0.4334]] | 2*t^2.099 + t^2.601 + t^2.898 + t^3.102 + 2*t^3.399 + t^3.696 + 4*t^4.198 + 3*t^4.7 + 2*t^4.997 + 2*t^5.201 + 4*t^5.498 + 3*t^5.795 - t^6. - t^4.3/y - t^4.3*y | detail |