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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56458 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6466 | 0.8094 | 0.7988 | [M:[1.1972, 1.0505, 0.8028, 0.8761, 1.1239, 0.7156, 1.0367], q:[0.4381, 0.3647], qb:[0.5114, 0.7592], phi:[0.4817]] | [M:[[10], [-38], [-10], [14], [-14], [16], [12]], q:[[7], [-17]], qb:[[31], [3]], phi:[[-6]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{6}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{2}$, ${ }M_{5}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{1}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ | ${}$ | -1 | t^2.147 + t^2.408 + t^2.628 + t^3.11 + t^3.151 + t^3.372 + t^3.592 + t^3.633 + t^3.812 + 2*t^4.073 + 2*t^4.293 + t^4.514 + t^4.555 + t^4.775 + t^4.817 + t^5.037 + 2*t^5.257 + t^5.298 + 2*t^5.518 + 2*t^5.738 + t^5.78 + t^5.959 - t^6. + t^6.041 + 2*t^6.22 + t^6.262 + t^6.303 + 2*t^6.44 + t^6.482 + t^6.523 + t^6.66 + 3*t^6.702 + t^6.743 + t^6.785 + 3*t^6.922 + t^6.963 + t^7.142 + 2*t^7.183 + t^7.225 + t^7.266 + 3*t^7.404 + 2*t^7.445 + t^7.624 + 3*t^7.665 + t^7.707 + 4*t^7.885 + t^7.927 + 2*t^8.105 + t^8.147 + t^8.325 + 3*t^8.367 - t^8.408 + 2*t^8.45 + 4*t^8.587 - t^8.628 + t^8.67 + 2*t^8.807 + 2*t^8.849 + t^8.89 + t^8.931 - t^4.445/y - t^6.592/y + t^7.293/y + t^7.555/y - t^7.596/y + t^7.775/y + t^8.037/y + t^8.257/y + (2*t^8.298)/y + (2*t^8.518)/y + t^8.56/y + t^8.738/y + (3*t^8.78)/y + t^8.959/y - t^4.445*y - t^6.592*y + t^7.293*y + t^7.555*y - t^7.596*y + t^7.775*y + t^8.037*y + t^8.257*y + 2*t^8.298*y + 2*t^8.518*y + t^8.56*y + t^8.738*y + 3*t^8.78*y + t^8.959*y | g1^16*t^2.147 + t^2.408/g1^10 + g1^14*t^2.628 + g1^12*t^3.11 + t^3.151/g1^38 + t^3.372/g1^14 + g1^10*t^3.592 + t^3.633/g1^40 + g1^34*t^3.812 + 2*g1^8*t^4.073 + 2*g1^32*t^4.293 + g1^56*t^4.514 + g1^6*t^4.555 + g1^30*t^4.775 + t^4.817/g1^20 + g1^4*t^5.037 + 2*g1^28*t^5.257 + t^5.298/g1^22 + 2*g1^2*t^5.518 + 2*g1^26*t^5.738 + t^5.78/g1^24 + g1^50*t^5.959 - t^6. + t^6.041/g1^50 + 2*g1^24*t^6.22 + t^6.262/g1^26 + t^6.303/g1^76 + 2*g1^48*t^6.44 + t^6.482/g1^2 + t^6.523/g1^52 + g1^72*t^6.66 + 3*g1^22*t^6.702 + t^6.743/g1^28 + t^6.785/g1^78 + 3*g1^46*t^6.922 + t^6.963/g1^4 + g1^70*t^7.142 + 2*g1^20*t^7.183 + t^7.225/g1^30 + t^7.266/g1^80 + 3*g1^44*t^7.404 + (2*t^7.445)/g1^6 + g1^68*t^7.624 + 3*g1^18*t^7.665 + t^7.707/g1^32 + 4*g1^42*t^7.885 + t^7.927/g1^8 + 2*g1^66*t^8.105 + g1^16*t^8.147 + g1^90*t^8.325 + 3*g1^40*t^8.367 - t^8.408/g1^10 + (2*t^8.45)/g1^60 + 4*g1^64*t^8.587 - g1^14*t^8.628 + t^8.67/g1^36 + 2*g1^88*t^8.807 + 2*g1^38*t^8.849 + t^8.89/g1^12 + t^8.931/g1^62 - t^4.445/(g1^6*y) - (g1^10*t^6.592)/y + (g1^32*t^7.293)/y + (g1^6*t^7.555)/y - t^7.596/(g1^44*y) + (g1^30*t^7.775)/y + (g1^4*t^8.037)/y + (g1^28*t^8.257)/y + (2*t^8.298)/(g1^22*y) + (2*g1^2*t^8.518)/y + t^8.56/(g1^48*y) + (g1^26*t^8.738)/y + (3*t^8.78)/(g1^24*y) + (g1^50*t^8.959)/y - (t^4.445*y)/g1^6 - g1^10*t^6.592*y + g1^32*t^7.293*y + g1^6*t^7.555*y - (t^7.596*y)/g1^44 + g1^30*t^7.775*y + g1^4*t^8.037*y + g1^28*t^8.257*y + (2*t^8.298*y)/g1^22 + 2*g1^2*t^8.518*y + (t^8.56*y)/g1^48 + g1^26*t^8.738*y + (3*t^8.78*y)/g1^24 + g1^50*t^8.959*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 |
---|---|---|---|---|---|---|---|---|---|
53305 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ | 0.6503 | 0.8152 | 0.7977 | [M:[1.2019, 1.0329, 0.7981, 0.8826, 1.1174, 0.723], q:[0.4413, 0.3568], qb:[0.5258, 0.7606], phi:[0.4789]] | t^2.169 + t^2.394 + t^2.648 + t^2.873 + t^3.099 + t^3.352 + t^3.578 + t^3.606 + t^3.859 + 2*t^4.084 + 2*t^4.338 + t^4.563 + t^4.591 + t^4.789 + t^4.817 + 2*t^5.042 + 2*t^5.268 + t^5.296 + 2*t^5.521 + 2*t^5.747 + t^5.775 + 2*t^5.972 - t^6. - t^4.437/y - t^4.437*y | detail |