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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6287 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{2}M_{6}$ + ${ }M_{5}M_{7}$ + ${ }M_{8}\phi_{1}^{2}$ + ${ }M_{9}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6633 | 0.8288 | 0.8003 | [M:[1.0534, 0.8275, 1.0595, 0.8214, 1.1786, 1.1725, 0.8214, 1.0595, 0.7084], q:[0.5328, 0.4137], qb:[0.4076, 0.7649], phi:[0.4702]] | [M:[[-30], [22], [4], [-12], [12], [-22], [-12], [4], [14]], q:[[19], [11]], qb:[[-23], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{9}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{8}$, ${ }M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{9}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}M_{9}$, ${ }M_{7}M_{9}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{9}$, ${ }M_{3}M_{9}$, ${ }M_{8}M_{9}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{7}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{6}M_{9}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{9}\phi_{1}\tilde{q}_{1}^{2}$ | ${}$ | -3 | t^2.125 + 2*t^2.464 + t^3.16 + 2*t^3.179 + t^3.518 + t^3.856 + 2*t^3.893 + t^4.232 + 2*t^4.25 + 2*t^4.589 + t^4.608 + 3*t^4.928 + t^5.285 + 2*t^5.304 + t^5.624 + 4*t^5.643 + 2*t^5.982 - 3*t^6. + t^6.018 + 3*t^6.32 + t^6.339 + 5*t^6.357 + t^6.376 + t^6.678 + 2*t^6.696 + 2*t^6.715 + t^6.733 + t^7.017 + t^7.035 + 2*t^7.053 + 3*t^7.072 + t^7.374 + 3*t^7.392 + 2*t^7.411 + 2*t^7.429 + t^7.713 + 2*t^7.75 + 3*t^7.768 + 2*t^7.786 + 2*t^8.088 + 5*t^8.107 - 3*t^8.125 + 2*t^8.144 + 4*t^8.446 - 4*t^8.464 + 2*t^8.482 + 3*t^8.501 + 4*t^8.785 + t^8.803 + 6*t^8.821 + t^8.84 + 2*t^8.858 - t^4.411/y - t^6.536/y - t^6.875/y + t^7.232/y + t^7.25/y - t^7.571/y + t^7.589/y + t^7.928/y + t^7.947/y + (2*t^8.285)/y + (2*t^8.304)/y + (2*t^8.624)/y + (5*t^8.643)/y - t^8.661/y + (3*t^8.982)/y - t^4.411*y - t^6.536*y - t^6.875*y + t^7.232*y + t^7.25*y - t^7.571*y + t^7.589*y + t^7.928*y + t^7.947*y + 2*t^8.285*y + 2*t^8.304*y + 2*t^8.624*y + 5*t^8.643*y - t^8.661*y + 3*t^8.982*y | g1^14*t^2.125 + (2*t^2.464)/g1^12 + t^3.16/g1^30 + 2*g1^4*t^3.179 + t^3.518/g1^22 + t^3.856/g1^48 + 2*g1^20*t^3.893 + t^4.232/g1^6 + 2*g1^28*t^4.25 + 2*g1^2*t^4.589 + g1^36*t^4.608 + (3*t^4.928)/g1^24 + t^5.285/g1^16 + 2*g1^18*t^5.304 + t^5.624/g1^42 + (4*t^5.643)/g1^8 + (2*t^5.982)/g1^34 - 3*t^6. + g1^34*t^6.018 + (3*t^6.32)/g1^60 + t^6.339/g1^26 + 5*g1^8*t^6.357 + g1^42*t^6.376 + t^6.678/g1^52 + (2*t^6.696)/g1^18 + 2*g1^16*t^6.715 + g1^50*t^6.733 + t^7.017/g1^78 + t^7.035/g1^44 + (2*t^7.053)/g1^10 + 3*g1^24*t^7.072 + t^7.374/g1^70 + (3*t^7.392)/g1^36 + (2*t^7.411)/g1^2 + 2*g1^32*t^7.429 + t^7.713/g1^96 + (2*t^7.75)/g1^28 + 3*g1^6*t^7.768 + 2*g1^40*t^7.786 + (2*t^8.088)/g1^54 + (5*t^8.107)/g1^20 - 3*g1^14*t^8.125 + 2*g1^48*t^8.144 + (4*t^8.446)/g1^46 - (4*t^8.464)/g1^12 + 2*g1^22*t^8.482 + 3*g1^56*t^8.501 + (4*t^8.785)/g1^72 + t^8.803/g1^38 + (6*t^8.821)/g1^4 + g1^30*t^8.84 + 2*g1^64*t^8.858 - t^4.411/(g1^2*y) - (g1^12*t^6.536)/y - t^6.875/(g1^14*y) + t^7.232/(g1^6*y) + (g1^28*t^7.25)/y - t^7.571/(g1^32*y) + (g1^2*t^7.589)/y + t^7.928/(g1^24*y) + (g1^10*t^7.947)/y + (2*t^8.285)/(g1^16*y) + (2*g1^18*t^8.304)/y + (2*t^8.624)/(g1^42*y) + (5*t^8.643)/(g1^8*y) - (g1^26*t^8.661)/y + (3*t^8.982)/(g1^34*y) - (t^4.411*y)/g1^2 - g1^12*t^6.536*y - (t^6.875*y)/g1^14 + (t^7.232*y)/g1^6 + g1^28*t^7.25*y - (t^7.571*y)/g1^32 + g1^2*t^7.589*y + (t^7.928*y)/g1^24 + g1^10*t^7.947*y + (2*t^8.285*y)/g1^16 + 2*g1^18*t^8.304*y + (2*t^8.624*y)/g1^42 + (5*t^8.643*y)/g1^8 - g1^26*t^8.661*y + (3*t^8.982*y)/g1^34 |
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 |
---|---|---|---|---|---|---|---|---|---|
4719 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{2}M_{6}$ + ${ }M_{5}M_{7}$ + ${ }M_{8}\phi_{1}^{2}$ | 0.6429 | 0.7905 | 0.8133 | [M:[1.0484, 0.8312, 1.0602, 0.8194, 1.1806, 1.1688, 0.8194, 1.0602], q:[0.536, 0.4156], qb:[0.4038, 0.7651], phi:[0.4699]] | 2*t^2.458 + t^3.145 + 2*t^3.181 + t^3.506 + t^3.832 + t^3.868 + 2*t^3.903 + t^4.229 + t^4.264 + t^4.626 + 3*t^4.916 + t^5.603 + 3*t^5.639 + t^5.965 - 3*t^6. - t^4.41/y - t^4.41*y | detail |