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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58924 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{2}^{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{7}\phi_{1}q_{1}^{2}$ + ${ }M_{6}M_{7}$ + ${ }M_{3}M_{8}$ | 0.7037 | 0.8784 | 0.8012 | [M:[0.9599, 1.0, 1.0401, 0.7143, 0.6742, 1.1429, 0.8571, 0.9599], q:[0.3571, 0.6829], qb:[0.6429, 0.6028], phi:[0.4286]] | [M:[[1], [0], [-1], [0], [1], [0], [0], [1]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{5}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{1}$, ${ }M_{8}$, ${ }M_{2}$, ${ }M_{6}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{5}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{1}M_{5}$, ${ }M_{5}M_{8}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{4}M_{8}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{7}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{7}M_{8}$, ${ }M_{4}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{8}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.023 + t^2.143 + t^2.571 + 2*t^2.88 + t^3. + t^3.429 + t^3.737 + t^4.045 + 2*t^4.166 + 2*t^4.286 + t^4.406 + t^4.594 + t^4.714 + 3*t^4.902 + 3*t^5.023 + 3*t^5.143 + t^5.383 + 3*t^5.451 + 2*t^5.571 + 3*t^5.76 + t^5.88 - 2*t^6. + t^6.068 - 2*t^6.12 + 2*t^6.188 - t^6.24 + 5*t^6.308 + 3*t^6.429 + 3*t^6.617 + 2*t^6.737 + 3*t^6.925 + 5*t^7.045 + 6*t^7.166 + 2*t^7.286 - t^7.406 + 5*t^7.474 + 4*t^7.594 + 4*t^7.714 + 5*t^7.782 + 5*t^7.902 + t^7.955 + 2*t^8.023 + t^8.091 - 3*t^8.143 + 2*t^8.211 - 3*t^8.263 + 7*t^8.331 + 5*t^8.451 - t^8.571 + 6*t^8.639 - 3*t^8.692 + 3*t^8.76 - t^8.812 - 3*t^8.88 + 3*t^8.948 - t^4.286/y - t^6.308/y - t^6.429/y - t^6.857/y + t^7.406/y + t^7.594/y + (2*t^7.714)/y + (2*t^7.902)/y + (3*t^8.023)/y + (2*t^8.143)/y + t^8.263/y - t^8.331/y + (2*t^8.451)/y + t^8.571/y + (2*t^8.76)/y + (2*t^8.88)/y - t^4.286*y - t^6.308*y - t^6.429*y - t^6.857*y + t^7.406*y + t^7.594*y + 2*t^7.714*y + 2*t^7.902*y + 3*t^8.023*y + 2*t^8.143*y + t^8.263*y - t^8.331*y + 2*t^8.451*y + t^8.571*y + 2*t^8.76*y + 2*t^8.88*y | g1*t^2.023 + t^2.143 + t^2.571 + 2*g1*t^2.88 + t^3. + t^3.429 + g1*t^3.737 + g1^2*t^4.045 + 2*g1*t^4.166 + 2*t^4.286 + t^4.406/g1 + g1*t^4.594 + t^4.714 + 3*g1^2*t^4.902 + 3*g1*t^5.023 + 3*t^5.143 + t^5.383/g1^2 + 3*g1*t^5.451 + 2*t^5.571 + 3*g1^2*t^5.76 + g1*t^5.88 - 2*t^6. + g1^3*t^6.068 - (2*t^6.12)/g1 + 2*g1^2*t^6.188 - t^6.24/g1^2 + 5*g1*t^6.308 + 3*t^6.429 + 3*g1^2*t^6.617 + 2*g1*t^6.737 + 3*g1^3*t^6.925 + 5*g1^2*t^7.045 + 6*g1*t^7.166 + 2*t^7.286 - t^7.406/g1 + 5*g1^2*t^7.474 + 4*g1*t^7.594 + 4*t^7.714 + 5*g1^3*t^7.782 + 5*g1^2*t^7.902 + t^7.955/g1^2 + 2*g1*t^8.023 + g1^4*t^8.091 - 3*t^8.143 + 2*g1^3*t^8.211 - (3*t^8.263)/g1 + 7*g1^2*t^8.331 + 5*g1*t^8.451 - t^8.571 + 6*g1^3*t^8.639 - (3*t^8.692)/g1 + 3*g1^2*t^8.76 - t^8.812/g1^2 - 3*g1*t^8.88 + 3*g1^4*t^8.948 - t^4.286/y - (g1*t^6.308)/y - t^6.429/y - t^6.857/y + t^7.406/(g1*y) + (g1*t^7.594)/y + (2*t^7.714)/y + (2*g1^2*t^7.902)/y + (3*g1*t^8.023)/y + (2*t^8.143)/y + t^8.263/(g1*y) - (g1^2*t^8.331)/y + (2*g1*t^8.451)/y + t^8.571/y + (2*g1^2*t^8.76)/y + (2*g1*t^8.88)/y - t^4.286*y - g1*t^6.308*y - t^6.429*y - t^6.857*y + (t^7.406*y)/g1 + g1*t^7.594*y + 2*t^7.714*y + 2*g1^2*t^7.902*y + 3*g1*t^8.023*y + 2*t^8.143*y + (t^8.263*y)/g1 - g1^2*t^8.331*y + 2*g1*t^8.451*y + t^8.571*y + 2*g1^2*t^8.76*y + 2*g1*t^8.88*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 |
---|---|---|---|---|---|---|---|---|---|
56990 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{2}^{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{7}\phi_{1}q_{1}^{2}$ + ${ }M_{6}M_{7}$ | 0.7015 | 0.8716 | 0.8048 | [M:[0.9914, 1.0, 1.0086, 0.7143, 0.7057, 1.1429, 0.8571], q:[0.3571, 0.6514], qb:[0.6429, 0.6343], phi:[0.4286]] | t^2.117 + t^2.143 + t^2.571 + t^2.974 + t^3. + t^3.026 + t^3.429 + t^3.831 + t^4.234 + 2*t^4.26 + 2*t^4.286 + t^4.311 + t^4.689 + t^4.714 + 2*t^5.091 + 2*t^5.117 + 4*t^5.143 + t^5.169 + t^5.194 + 2*t^5.546 + 2*t^5.571 + t^5.597 + t^5.949 - t^6. - t^4.286/y - t^4.286*y | detail |