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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2470 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{3}M_{7}$ | 0.7165 | 0.8891 | 0.8059 | [M:[1.0, 0.9053, 1.0947, 0.8105, 1.0, 0.9053, 0.9053], q:[0.4526, 0.5474], qb:[0.4526, 0.6421], phi:[0.4763]] | [M:[[0], [-4], [4], [-8], [0], [-4], [-4]], q:[[-2], [2]], qb:[[-2], [6]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }M_{2}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{4}M_{7}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$ | ${}M_{1}M_{5}$ | -3 | t^2.432 + 3*t^2.716 + t^2.858 + 2*t^3. + 3*t^4.145 + 2*t^4.429 + 3*t^4.713 + t^4.863 + t^4.997 + 3*t^5.147 + t^5.282 + t^5.289 + 6*t^5.432 + 3*t^5.574 + 4*t^5.716 + 2*t^5.858 - 3*t^6. - 4*t^6.284 - 2*t^6.568 + 3*t^6.576 + 9*t^6.86 + 3*t^7.003 + 10*t^7.145 - t^7.287 + t^7.295 + 6*t^7.429 + t^7.571 + 3*t^7.579 + 2*t^7.713 + t^7.721 - 2*t^7.855 + 6*t^7.863 + 3*t^8.005 + 9*t^8.147 + 11*t^8.289 - t^8.424 + t^8.432 + 8*t^8.574 - 13*t^8.716 + 4*t^8.858 - t^4.429/y - t^6.86/y - (2*t^7.145)/y - t^7.287/y + t^7.571/y + (2*t^7.713)/y + t^7.997/y + (3*t^8.147)/y + t^8.289/y + (5*t^8.432)/y + (3*t^8.574)/y + (6*t^8.716)/y + (2*t^8.858)/y - t^4.429*y - t^6.86*y - 2*t^7.145*y - t^7.287*y + t^7.571*y + 2*t^7.713*y + t^7.997*y + 3*t^8.147*y + t^8.289*y + 5*t^8.432*y + 3*t^8.574*y + 6*t^8.716*y + 2*t^8.858*y | t^2.432/g1^8 + (3*t^2.716)/g1^4 + t^2.858/g1^2 + 2*t^3. + (3*t^4.145)/g1^5 + (2*t^4.429)/g1 + 3*g1^3*t^4.713 + t^4.863/g1^16 + g1^7*t^4.997 + (3*t^5.147)/g1^12 + g1^11*t^5.282 + t^5.289/g1^10 + (6*t^5.432)/g1^8 + (3*t^5.574)/g1^6 + (4*t^5.716)/g1^4 + (2*t^5.858)/g1^2 - 3*t^6. - 4*g1^4*t^6.284 - 2*g1^8*t^6.568 + (3*t^6.576)/g1^13 + (9*t^6.86)/g1^9 + (3*t^7.003)/g1^7 + (10*t^7.145)/g1^5 - t^7.287/g1^3 + t^7.295/g1^24 + (6*t^7.429)/g1 + g1*t^7.571 + (3*t^7.579)/g1^20 + 2*g1^3*t^7.713 + t^7.721/g1^18 - 2*g1^5*t^7.855 + (6*t^7.863)/g1^16 + (3*t^8.005)/g1^14 + (9*t^8.147)/g1^12 + (11*t^8.289)/g1^10 - g1^13*t^8.424 + t^8.432/g1^8 + (8*t^8.574)/g1^6 - (13*t^8.716)/g1^4 + (4*t^8.858)/g1^2 - t^4.429/(g1*y) - t^6.86/(g1^9*y) - (2*t^7.145)/(g1^5*y) - t^7.287/(g1^3*y) + (g1*t^7.571)/y + (2*g1^3*t^7.713)/y + (g1^7*t^7.997)/y + (3*t^8.147)/(g1^12*y) + t^8.289/(g1^10*y) + (5*t^8.432)/(g1^8*y) + (3*t^8.574)/(g1^6*y) + (6*t^8.716)/(g1^4*y) + (2*t^8.858)/(g1^2*y) - (t^4.429*y)/g1 - (t^6.86*y)/g1^9 - (2*t^7.145*y)/g1^5 - (t^7.287*y)/g1^3 + g1*t^7.571*y + 2*g1^3*t^7.713*y + g1^7*t^7.997*y + (3*t^8.147*y)/g1^12 + (t^8.289*y)/g1^10 + (5*t^8.432*y)/g1^8 + (3*t^8.574*y)/g1^6 + (6*t^8.716*y)/g1^4 + (2*t^8.858*y)/g1^2 |
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 |
---|---|---|---|---|---|---|---|---|---|
1402 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ | 0.7086 | 0.8735 | 0.8112 | [M:[1.0, 0.9207, 1.0793, 0.8413, 1.0, 0.9207], q:[0.4603, 0.5397], qb:[0.4603, 0.619], phi:[0.4802]] | t^2.524 + 2*t^2.762 + t^2.881 + 2*t^3. + t^3.238 + 3*t^4.202 + 2*t^4.44 + 3*t^4.679 + t^4.917 + t^5.048 + t^5.155 + 2*t^5.286 + t^5.405 + 3*t^5.524 + 2*t^5.643 + 3*t^5.762 + 2*t^5.881 - t^6. - t^4.44/y - t^4.44*y | detail |