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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56923 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{7}\phi_{1}q_{1}^{2}$ | 0.6847 | 0.8722 | 0.785 | [M:[1.2096, 0.8384, 0.7904, 0.8384, 0.8864, 0.7904, 0.7424], q:[0.4192, 0.3712], qb:[0.7424, 0.7904], phi:[0.4192]] | [M:[[-1], [-4], [1], [-4], [-9], [1], [6]], q:[[-2], [3]], qb:[[6], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{7}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{2}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}$, ${ }M_{7}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$ | 1 | t^2.227 + 2*t^2.371 + 3*t^2.515 + t^2.659 + t^3.485 + t^3.629 + t^4.454 + 4*t^4.598 + 7*t^4.742 + 6*t^4.886 + 7*t^5.03 + 3*t^5.174 + t^5.318 + 2*t^5.712 + 2*t^5.856 + t^6. + t^6.682 + 4*t^6.826 + 8*t^6.97 + 12*t^7.114 + 14*t^7.258 + 13*t^7.402 + 14*t^7.546 + 7*t^7.69 + 3*t^7.833 + 2*t^7.939 + t^7.977 + 3*t^8.083 + 2*t^8.227 - 5*t^8.371 - 6*t^8.515 - 5*t^8.659 - 3*t^8.803 + t^8.909 - t^4.258/y - t^6.485/y - t^6.629/y - (3*t^6.773)/y - t^6.917/y + (3*t^7.598)/y + (7*t^7.742)/y + (8*t^7.886)/y + (6*t^8.03)/y + (3*t^8.174)/y + (2*t^8.856)/y - t^4.258*y - t^6.485*y - t^6.629*y - 3*t^6.773*y - t^6.917*y + 3*t^7.598*y + 7*t^7.742*y + 8*t^7.886*y + 6*t^8.03*y + 3*t^8.174*y + 2*t^8.856*y | g1^6*t^2.227 + 2*g1*t^2.371 + (3*t^2.515)/g1^4 + t^2.659/g1^9 + g1^4*t^3.485 + t^3.629/g1 + g1^12*t^4.454 + 4*g1^7*t^4.598 + 7*g1^2*t^4.742 + (6*t^4.886)/g1^3 + (7*t^5.03)/g1^8 + (3*t^5.174)/g1^13 + t^5.318/g1^18 + 2*g1^10*t^5.712 + 2*g1^5*t^5.856 + t^6. + g1^18*t^6.682 + 4*g1^13*t^6.826 + 8*g1^8*t^6.97 + 12*g1^3*t^7.114 + (14*t^7.258)/g1^2 + (13*t^7.402)/g1^7 + (14*t^7.546)/g1^12 + (7*t^7.69)/g1^17 + (3*t^7.833)/g1^22 + 2*g1^16*t^7.939 + t^7.977/g1^27 + 3*g1^11*t^8.083 + 2*g1^6*t^8.227 - 5*g1*t^8.371 - (6*t^8.515)/g1^4 - (5*t^8.659)/g1^9 - (3*t^8.803)/g1^14 + g1^24*t^8.909 - t^4.258/(g1^2*y) - (g1^4*t^6.485)/y - t^6.629/(g1*y) - (3*t^6.773)/(g1^6*y) - t^6.917/(g1^11*y) + (3*g1^7*t^7.598)/y + (7*g1^2*t^7.742)/y + (8*t^7.886)/(g1^3*y) + (6*t^8.03)/(g1^8*y) + (3*t^8.174)/(g1^13*y) + (2*g1^5*t^8.856)/y - (t^4.258*y)/g1^2 - g1^4*t^6.485*y - (t^6.629*y)/g1 - (3*t^6.773*y)/g1^6 - (t^6.917*y)/g1^11 + 3*g1^7*t^7.598*y + 7*g1^2*t^7.742*y + (8*t^7.886*y)/g1^3 + (6*t^8.03*y)/g1^8 + (3*t^8.174*y)/g1^13 + 2*g1^5*t^8.856*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 |
---|---|---|---|---|---|---|---|---|---|
55268 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}M_{6}$ | 0.6656 | 0.8379 | 0.7944 | [M:[1.2072, 0.829, 0.7928, 0.829, 0.8652, 0.7928], q:[0.4145, 0.3783], qb:[0.7566, 0.7928], phi:[0.4145]] | 2*t^2.378 + 3*t^2.487 + t^2.596 + t^3.513 + t^3.622 + t^3.73 + 2*t^4.648 + 4*t^4.757 + 5*t^4.865 + 7*t^4.974 + 3*t^5.082 + t^5.191 + t^5.783 + t^5.891 + t^6. - t^4.243/y - t^4.243*y | detail |