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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2729 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ | 0.5633 | 0.7261 | 0.7758 | [M:[1.1316, 0.7764, 0.9605, 0.6973], q:[0.5658, 1.0], qb:[0.3027, 0.3947], phi:[0.4342]] | [M:[[2], [-11], [7], [3]], q:[[1], [0]], qb:[[-3], [6]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}^{4}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}$ | -2 | 2*t^2.092 + t^2.329 + t^2.605 + 2*t^2.881 + 2*t^3.395 + 4*t^4.184 + 2*t^4.421 + t^4.659 + 3*t^4.697 + t^4.935 + 4*t^4.973 + 2*t^5.211 + 5*t^5.487 + t^5.724 + 3*t^5.763 - 2*t^6. + 8*t^6.276 + t^6.513 + 2*t^6.751 + 4*t^6.789 + t^6.988 + 2*t^7.027 + 7*t^7.065 + t^7.264 + t^7.303 + 2*t^7.54 + 9*t^7.579 + t^7.816 + 6*t^7.855 + t^8.053 - 3*t^8.092 - 3*t^8.329 + 13*t^8.368 - 2*t^8.605 + 4*t^8.644 + t^8.843 - t^8.881 - t^4.303/y - t^6.395/y - t^6.632/y + (3*t^7.421)/y + (2*t^7.697)/y + t^7.935/y + (5*t^7.973)/y + (3*t^8.211)/y + (5*t^8.487)/y + t^8.724/y + t^8.763/y - t^8.961/y - t^4.303*y - t^6.395*y - t^6.632*y + 3*t^7.421*y + 2*t^7.697*y + t^7.935*y + 5*t^7.973*y + 3*t^8.211*y + 5*t^8.487*y + t^8.724*y + t^8.763*y - t^8.961*y | 2*g1^3*t^2.092 + t^2.329/g1^11 + t^2.605/g1^2 + 2*g1^7*t^2.881 + 2*g1^2*t^3.395 + 4*g1^6*t^4.184 + (2*t^4.421)/g1^8 + t^4.659/g1^22 + 3*g1*t^4.697 + t^4.935/g1^13 + 4*g1^10*t^4.973 + (2*t^5.211)/g1^4 + 5*g1^5*t^5.487 + t^5.724/g1^9 + 3*g1^14*t^5.763 - 2*t^6. + 8*g1^9*t^6.276 + t^6.513/g1^5 + (2*t^6.751)/g1^19 + 4*g1^4*t^6.789 + t^6.988/g1^33 + (2*t^7.027)/g1^10 + 7*g1^13*t^7.065 + t^7.264/g1^24 + t^7.303/g1 + (2*t^7.54)/g1^15 + 9*g1^8*t^7.579 + t^7.816/g1^6 + 6*g1^17*t^7.855 + t^8.053/g1^20 - 3*g1^3*t^8.092 - (3*t^8.329)/g1^11 + 13*g1^12*t^8.368 - (2*t^8.605)/g1^2 + 4*g1^21*t^8.644 + t^8.843/g1^16 - g1^7*t^8.881 - t^4.303/(g1*y) - (g1^2*t^6.395)/y - t^6.632/(g1^12*y) + (3*t^7.421)/(g1^8*y) + (2*g1*t^7.697)/y + t^7.935/(g1^13*y) + (5*g1^10*t^7.973)/y + (3*t^8.211)/(g1^4*y) + (5*g1^5*t^8.487)/y + t^8.724/(g1^9*y) + (g1^14*t^8.763)/y - t^8.961/(g1^23*y) - (t^4.303*y)/g1 - g1^2*t^6.395*y - (t^6.632*y)/g1^12 + (3*t^7.421*y)/g1^8 + 2*g1*t^7.697*y + (t^7.935*y)/g1^13 + 5*g1^10*t^7.973*y + (3*t^8.211*y)/g1^4 + 5*g1^5*t^8.487*y + (t^8.724*y)/g1^9 + g1^14*t^8.763*y - (t^8.961*y)/g1^23 |
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 |
---|---|---|---|---|---|---|---|---|---|
1730 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 0.5427 | 0.6866 | 0.7905 | [M:[1.1322, 0.7727, 0.9628], q:[0.5661, 1.0], qb:[0.3017, 0.3967], phi:[0.4339]] | t^2.095 + t^2.318 + t^2.603 + 2*t^2.888 + 2*t^3.397 + t^3.905 + 2*t^4.19 + t^4.413 + t^4.636 + 2*t^4.698 + t^4.922 + 2*t^4.983 + 2*t^5.207 + 3*t^5.492 + t^5.715 + 3*t^5.777 - t^6. - t^4.302/y - t^4.302*y | detail |