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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56807 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{2}M_{7}$ | 0.693 | 0.8533 | 0.8121 | [M:[0.9716, 1.017, 1.0284, 0.9943, 0.983, 0.9716, 0.983], q:[0.4972, 0.5312], qb:[0.4858, 0.4744], phi:[0.5028]] | [M:[[10], [-6], [-10], [2], [6], [10], [6]], q:[[1], [-11]], qb:[[5], [9]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }M_{6}$, ${ }M_{5}$, ${ }M_{7}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$ | ${}$ | -3 | t^2.881 + 2*t^2.915 + 2*t^2.949 + t^2.983 + t^3.017 + t^4.355 + t^4.389 + 2*t^4.423 + t^4.457 + t^4.491 + t^4.526 + t^4.56 + t^4.594 + t^4.696 + t^5.761 + 2*t^5.796 + 4*t^5.83 + 4*t^5.864 + 5*t^5.898 + 3*t^5.932 - 3*t^6. - t^6.034 - t^6.068 - t^6.102 - t^6.136 - t^6.17 + t^7.236 + 3*t^7.27 + 5*t^7.304 + 5*t^7.338 + 6*t^7.372 + 4*t^7.406 + 4*t^7.44 + t^7.474 + t^7.611 - t^7.679 + t^7.713 + t^8.642 + 2*t^8.676 + 5*t^8.71 + 7*t^8.744 + 10*t^8.779 + 10*t^8.813 + 8*t^8.847 - 5*t^8.915 - 7*t^8.949 - 6*t^8.983 - t^4.509/y - t^7.423/y - t^7.457/y + t^7.56/y + t^7.594/y + (2*t^8.796)/y + (3*t^8.83)/y + (5*t^8.864)/y + (4*t^8.898)/y + (4*t^8.932)/y + (2*t^8.966)/y - t^4.509*y - t^7.423*y - t^7.457*y + t^7.56*y + t^7.594*y + 2*t^8.796*y + 3*t^8.83*y + 5*t^8.864*y + 4*t^8.898*y + 4*t^8.932*y + 2*t^8.966*y | g1^14*t^2.881 + 2*g1^10*t^2.915 + 2*g1^6*t^2.949 + g1^2*t^2.983 + t^3.017/g1^2 + g1^17*t^4.355 + g1^13*t^4.389 + 2*g1^9*t^4.423 + g1^5*t^4.457 + g1*t^4.491 + t^4.526/g1^3 + t^4.56/g1^7 + t^4.594/g1^11 + t^4.696/g1^23 + g1^28*t^5.761 + 2*g1^24*t^5.796 + 4*g1^20*t^5.83 + 4*g1^16*t^5.864 + 5*g1^12*t^5.898 + 3*g1^8*t^5.932 - 3*t^6. - t^6.034/g1^4 - t^6.068/g1^8 - t^6.102/g1^12 - t^6.136/g1^16 - t^6.17/g1^20 + g1^31*t^7.236 + 3*g1^27*t^7.27 + 5*g1^23*t^7.304 + 5*g1^19*t^7.338 + 6*g1^15*t^7.372 + 4*g1^11*t^7.406 + 4*g1^7*t^7.44 + g1^3*t^7.474 + t^7.611/g1^13 - t^7.679/g1^21 + t^7.713/g1^25 + g1^42*t^8.642 + 2*g1^38*t^8.676 + 5*g1^34*t^8.71 + 7*g1^30*t^8.744 + 10*g1^26*t^8.779 + 10*g1^22*t^8.813 + 8*g1^18*t^8.847 - 5*g1^10*t^8.915 - 7*g1^6*t^8.949 - 6*g1^2*t^8.983 - t^4.509/(g1*y) - (g1^9*t^7.423)/y - (g1^5*t^7.457)/y + t^7.56/(g1^7*y) + t^7.594/(g1^11*y) + (2*g1^24*t^8.796)/y + (3*g1^20*t^8.83)/y + (5*g1^16*t^8.864)/y + (4*g1^12*t^8.898)/y + (4*g1^8*t^8.932)/y + (2*g1^4*t^8.966)/y - (t^4.509*y)/g1 - g1^9*t^7.423*y - g1^5*t^7.457*y + (t^7.56*y)/g1^7 + (t^7.594*y)/g1^11 + 2*g1^24*t^8.796*y + 3*g1^20*t^8.83*y + 5*g1^16*t^8.864*y + 4*g1^12*t^8.898*y + 4*g1^8*t^8.932*y + 2*g1^4*t^8.966*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 |
---|---|---|---|---|---|---|---|---|---|
55126 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ | 0.6918 | 0.8495 | 0.8143 | [M:[0.9861, 1.0084, 1.0139, 0.9972, 0.9916, 0.9861], q:[0.4986, 0.5153], qb:[0.493, 0.4875], phi:[0.5014]] | t^2.942 + 2*t^2.958 + t^2.975 + t^2.992 + t^3.008 + t^3.025 + t^4.429 + t^4.446 + 2*t^4.462 + t^4.479 + t^4.496 + t^4.513 + t^4.529 + t^4.546 + t^4.596 + t^5.883 + 2*t^5.9 + 3*t^5.916 + 2*t^5.933 + 3*t^5.95 + 3*t^5.967 + t^5.983 - 2*t^6. - t^4.504/y - t^4.504*y | detail |