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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5263 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{3}X_{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}M_{7}$ + ${ }M_{8}\phi_{1}\tilde{q}_{2}^{2}$ | 0.5872 | 0.7255 | 0.8093 | [X:[1.6, 1.3861], M:[0.4, 1.2, 0.6139, 0.9861, 1.0139, 0.8277, 0.9861, 0.7723], q:[1.0, 0.6], qb:[0.3861, 0.4139], phi:[0.4]] | [X:[[0], [1]], M:[[0], [0], [-1], [1], [-1], [-2], [1], [2]], q:[[0], [0]], qb:[[1], [-1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }X_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{8}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{6}M_{8}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }X_{1}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{2}M_{8}$, ${ }M_{8}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{1}^{2}q_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.317 + t^2.4 + t^2.483 + 2*t^2.958 + 2*t^3.6 + t^4.158 + t^4.242 + t^4.634 + t^4.717 + 3*t^4.8 + t^4.883 + t^4.966 + 2*t^5.275 + t^5.358 + t^5.442 + 4*t^5.917 - t^6. + t^6.083 + t^6.475 + 3*t^6.558 - t^6.642 + t^6.725 + t^6.95 + t^7.034 + 3*t^7.117 + 3*t^7.2 + t^7.283 + t^7.366 + t^7.45 + 2*t^7.592 + t^7.675 + 3*t^7.758 - t^7.842 + t^7.925 + 4*t^8.234 - t^8.317 + 2*t^8.4 - 2*t^8.483 + t^8.566 + t^8.792 + 5*t^8.875 - 4*t^8.958 - t^4.2/y - t^6.517/y - t^6.683/y - t^7.158/y + t^7.242/y + (2*t^7.717)/y + t^7.8/y + (2*t^7.883)/y + (2*t^8.275)/y + (2*t^8.358)/y + (2*t^8.442)/y - t^8.834/y + (3*t^8.917)/y - t^4.2*y - t^6.517*y - t^6.683*y - t^7.158*y + t^7.242*y + 2*t^7.717*y + t^7.8*y + 2*t^7.883*y + 2*t^8.275*y + 2*t^8.358*y + 2*t^8.442*y - t^8.834*y + 3*t^8.917*y | g1^2*t^2.317 + t^2.4 + t^2.483/g1^2 + 2*g1*t^2.958 + 2*t^3.6 + g1*t^4.158 + t^4.242/g1 + g1^4*t^4.634 + g1^2*t^4.717 + 3*t^4.8 + t^4.883/g1^2 + t^4.966/g1^4 + 2*g1^3*t^5.275 + g1*t^5.358 + t^5.442/g1 + 4*g1^2*t^5.917 - t^6. + t^6.083/g1^2 + g1^3*t^6.475 + 3*g1*t^6.558 - t^6.642/g1 + t^6.725/g1^3 + g1^6*t^6.95 + g1^4*t^7.034 + 3*g1^2*t^7.117 + 3*t^7.2 + t^7.283/g1^2 + t^7.366/g1^4 + t^7.45/g1^6 + 2*g1^5*t^7.592 + g1^3*t^7.675 + 3*g1*t^7.758 - t^7.842/g1 + t^7.925/g1^3 + 4*g1^4*t^8.234 - g1^2*t^8.317 + 2*t^8.4 - (2*t^8.483)/g1^2 + t^8.566/g1^4 + g1^5*t^8.792 + 5*g1^3*t^8.875 - 4*g1*t^8.958 - t^4.2/y - (g1^2*t^6.517)/y - t^6.683/(g1^2*y) - (g1*t^7.158)/y + t^7.242/(g1*y) + (2*g1^2*t^7.717)/y + t^7.8/y + (2*t^7.883)/(g1^2*y) + (2*g1^3*t^8.275)/y + (2*g1*t^8.358)/y + (2*t^8.442)/(g1*y) - (g1^4*t^8.834)/y + (3*g1^2*t^8.917)/y - t^4.2*y - g1^2*t^6.517*y - (t^6.683*y)/g1^2 - g1*t^7.158*y + (t^7.242*y)/g1 + 2*g1^2*t^7.717*y + t^7.8*y + (2*t^7.883*y)/g1^2 + 2*g1^3*t^8.275*y + 2*g1*t^8.358*y + (2*t^8.442*y)/g1 - g1^4*t^8.834*y + 3*g1^2*t^8.917*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 |
---|---|---|---|---|---|---|---|---|---|
3589 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{3}X_{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}M_{7}$ | 0.5701 | 0.6954 | 0.8198 | [X:[1.6, 1.4048], M:[0.4, 1.2, 0.5952, 1.0048, 0.9952, 0.7903, 1.0048], q:[1.0, 0.6], qb:[0.4048, 0.3952], phi:[0.4]] | t^2.371 + t^2.4 + 2*t^3.015 + t^3.571 + 2*t^3.6 + t^4.185 + t^4.215 + t^4.742 + t^4.771 + 2*t^4.8 + t^5.385 + t^5.415 + t^5.942 + 2*t^5.971 - t^6. - t^4.2/y - t^4.2*y | detail |