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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4575 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{1}M_{7}$ + ${ }M_{5}M_{8}$ | 0.6971 | 0.8572 | 0.8133 | [M:[1.0111, 0.9667, 1.0333, 0.9445, 1.0555, 0.9667, 0.9889, 0.9445], q:[0.5055, 0.4834], qb:[0.4612, 0.5721], phi:[0.4945]] | [M:[[2], [-6], [6], [-10], [10], [-6], [-2], [-10]], q:[[1], [-3]], qb:[[-7], [13]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }M_{8}$, ${ }M_{2}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{2}M_{8}$, ${ }M_{6}M_{8}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$ | ${}$ | -4 | 2*t^2.834 + 2*t^2.9 + 2*t^2.967 + t^3.233 + t^4.25 + t^4.317 + 2*t^4.383 + t^4.45 + t^4.517 + t^4.583 + t^4.65 + t^4.716 + t^4.916 + 2*t^5.667 + 3*t^5.734 + 6*t^5.8 + 3*t^5.867 + t^5.933 - 4*t^6. - t^6.067 + t^6.133 + t^6.2 - t^6.266 - t^6.333 + t^6.466 + 2*t^7.084 + 3*t^7.15 + 6*t^7.217 + 5*t^7.284 + 5*t^7.35 + t^7.417 + t^7.483 + t^7.55 + 2*t^7.617 + t^7.816 + 2*t^7.883 + t^8.149 + 3*t^8.501 + 4*t^8.567 + 9*t^8.634 + 8*t^8.7 + 8*t^8.767 - 3*t^8.834 - 7*t^8.9 - 8*t^8.967 - t^4.483/y - t^7.317/y - t^7.383/y - t^7.45/y + t^7.517/y + t^7.583/y + t^7.65/y + t^8.667/y + (4*t^8.734)/y + (5*t^8.8)/y + (4*t^8.867)/y + t^8.933/y - t^4.483*y - t^7.317*y - t^7.383*y - t^7.45*y + t^7.517*y + t^7.583*y + t^7.65*y + t^8.667*y + 4*t^8.734*y + 5*t^8.8*y + 4*t^8.867*y + t^8.933*y | (2*t^2.834)/g1^10 + (2*t^2.9)/g1^6 + (2*t^2.967)/g1^2 + g1^14*t^3.233 + t^4.25/g1^15 + t^4.317/g1^11 + (2*t^4.383)/g1^7 + t^4.45/g1^3 + g1*t^4.517 + g1^5*t^4.583 + g1^9*t^4.65 + g1^13*t^4.716 + g1^25*t^4.916 + (2*t^5.667)/g1^20 + (3*t^5.734)/g1^16 + (6*t^5.8)/g1^12 + (3*t^5.867)/g1^8 + t^5.933/g1^4 - 4*t^6. - g1^4*t^6.067 + g1^8*t^6.133 + g1^12*t^6.2 - g1^16*t^6.266 - g1^20*t^6.333 + g1^28*t^6.466 + (2*t^7.084)/g1^25 + (3*t^7.15)/g1^21 + (6*t^7.217)/g1^17 + (5*t^7.284)/g1^13 + (5*t^7.35)/g1^9 + t^7.417/g1^5 + t^7.483/g1 + g1^3*t^7.55 + 2*g1^7*t^7.617 + g1^19*t^7.816 + 2*g1^23*t^7.883 + g1^39*t^8.149 + (3*t^8.501)/g1^30 + (4*t^8.567)/g1^26 + (9*t^8.634)/g1^22 + (8*t^8.7)/g1^18 + (8*t^8.767)/g1^14 - (3*t^8.834)/g1^10 - (7*t^8.9)/g1^6 - (8*t^8.967)/g1^2 - t^4.483/(g1*y) - t^7.317/(g1^11*y) - t^7.383/(g1^7*y) - t^7.45/(g1^3*y) + (g1*t^7.517)/y + (g1^5*t^7.583)/y + (g1^9*t^7.65)/y + t^8.667/(g1^20*y) + (4*t^8.734)/(g1^16*y) + (5*t^8.8)/(g1^12*y) + (4*t^8.867)/(g1^8*y) + t^8.933/(g1^4*y) - (t^4.483*y)/g1 - (t^7.317*y)/g1^11 - (t^7.383*y)/g1^7 - (t^7.45*y)/g1^3 + g1*t^7.517*y + g1^5*t^7.583*y + g1^9*t^7.65*y + (t^8.667*y)/g1^20 + (4*t^8.734*y)/g1^16 + (5*t^8.8*y)/g1^12 + (4*t^8.867*y)/g1^8 + (t^8.933*y)/g1^4 |
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 |
---|---|---|---|---|---|---|---|---|---|
2521 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{1}M_{7}$ | 0.6931 | 0.8496 | 0.8159 | [M:[1.0061, 0.9818, 1.0182, 0.9697, 1.0303, 0.9818, 0.9939], q:[0.503, 0.4909], qb:[0.4788, 0.5394], phi:[0.497]] | t^2.909 + 2*t^2.945 + 2*t^2.982 + t^3.091 + t^3.127 + t^4.363 + t^4.4 + 2*t^4.436 + t^4.473 + t^4.509 + t^4.546 + t^4.582 + t^4.618 + t^4.728 + t^5.854 + 4*t^5.891 + 3*t^5.927 + t^5.964 - 3*t^6. - t^4.491/y - t^4.491*y | detail |