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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2870 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{1}M_{6}$ | 0.677 | 0.851 | 0.7956 | [M:[1.1331, 0.7415, 0.8669, 0.8669, 0.6997, 0.8669], q:[0.8042, 0.4961], qb:[0.3708, 0.7624], phi:[0.3916]] | [M:[[16], [14], [-16], [-16], [24], [-16]], q:[[-1], [-23]], qb:[[7], [9]], phi:[[2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{5}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}^{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ | ${}$ | -3 | t^2.099 + t^2.225 + t^2.35 + 3*t^2.601 + t^3.525 + t^3.775 + t^4.152 + t^4.198 + t^4.324 + 2*t^4.449 + 2*t^4.574 + 5*t^4.7 + 2*t^4.825 + 4*t^4.95 + 5*t^5.201 + 2*t^5.749 + t^5.875 - 3*t^6. + 3*t^6.125 + t^6.297 + 2*t^6.376 + t^6.423 + t^6.501 + 2*t^6.548 + 3*t^6.674 + 3*t^6.752 + 5*t^6.799 + 4*t^6.924 + 7*t^7.05 + 2*t^7.175 + 10*t^7.3 + 2*t^7.426 + 6*t^7.551 + 6*t^7.802 + t^7.848 + t^7.927 + t^7.974 - 2*t^8.099 - 2*t^8.225 + t^8.303 - 2*t^8.35 + t^8.397 + 2*t^8.475 + t^8.522 - 10*t^8.601 + 2*t^8.647 + 5*t^8.726 + 3*t^8.773 + t^8.851 + 6*t^8.898 + 2*t^8.977 - t^4.175/y - t^6.274/y - t^6.399/y - t^6.525/y - (2*t^6.775)/y + t^7.324/y + t^7.449/y + (3*t^7.574)/y + (3*t^7.7)/y + (4*t^7.825)/y + (4*t^7.95)/y + t^8.076/y + (3*t^8.201)/y - t^8.373/y - t^8.499/y - t^8.624/y - t^8.875/y - t^4.175*y - t^6.274*y - t^6.399*y - t^6.525*y - 2*t^6.775*y + t^7.324*y + t^7.449*y + 3*t^7.574*y + 3*t^7.7*y + 4*t^7.825*y + 4*t^7.95*y + t^8.076*y + 3*t^8.201*y - t^8.373*y - t^8.499*y - t^8.624*y - t^8.875*y | g1^24*t^2.099 + g1^14*t^2.225 + g1^4*t^2.35 + (3*t^2.601)/g1^16 + g1^6*t^3.525 + t^3.775/g1^14 + t^4.152/g1^44 + g1^48*t^4.198 + g1^38*t^4.324 + 2*g1^28*t^4.449 + 2*g1^18*t^4.574 + 5*g1^8*t^4.7 + (2*t^4.825)/g1^2 + (4*t^4.95)/g1^12 + (5*t^5.201)/g1^32 + 2*g1^20*t^5.749 + g1^10*t^5.875 - 3*t^6. + (3*t^6.125)/g1^10 + g1^72*t^6.297 + (2*t^6.376)/g1^30 + g1^62*t^6.423 + t^6.501/g1^40 + 2*g1^52*t^6.548 + 3*g1^42*t^6.674 + (3*t^6.752)/g1^60 + 5*g1^32*t^6.799 + 4*g1^22*t^6.924 + 7*g1^12*t^7.05 + 2*g1^2*t^7.175 + (10*t^7.3)/g1^8 + (2*t^7.426)/g1^18 + (6*t^7.551)/g1^28 + (6*t^7.802)/g1^48 + g1^44*t^7.848 + t^7.927/g1^58 + g1^34*t^7.974 - 2*g1^24*t^8.099 - 2*g1^14*t^8.225 + t^8.303/g1^88 - 2*g1^4*t^8.35 + g1^96*t^8.397 + (2*t^8.475)/g1^6 + g1^86*t^8.522 - (10*t^8.601)/g1^16 + 2*g1^76*t^8.647 + (5*t^8.726)/g1^26 + 3*g1^66*t^8.773 + t^8.851/g1^36 + 6*g1^56*t^8.898 + (2*t^8.977)/g1^46 - (g1^2*t^4.175)/y - (g1^26*t^6.274)/y - (g1^16*t^6.399)/y - (g1^6*t^6.525)/y - (2*t^6.775)/(g1^14*y) + (g1^38*t^7.324)/y + (g1^28*t^7.449)/y + (3*g1^18*t^7.574)/y + (3*g1^8*t^7.7)/y + (4*t^7.825)/(g1^2*y) + (4*t^7.95)/(g1^12*y) + t^8.076/(g1^22*y) + (3*t^8.201)/(g1^32*y) - (g1^50*t^8.373)/y - (g1^40*t^8.499)/y - (g1^30*t^8.624)/y - (g1^10*t^8.875)/y - g1^2*t^4.175*y - g1^26*t^6.274*y - g1^16*t^6.399*y - g1^6*t^6.525*y - (2*t^6.775*y)/g1^14 + g1^38*t^7.324*y + g1^28*t^7.449*y + 3*g1^18*t^7.574*y + 3*g1^8*t^7.7*y + (4*t^7.825*y)/g1^2 + (4*t^7.95*y)/g1^12 + (t^8.076*y)/g1^22 + (3*t^8.201*y)/g1^32 - g1^50*t^8.373*y - g1^40*t^8.499*y - g1^30*t^8.624*y - g1^10*t^8.875*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 |
---|---|---|---|---|---|---|---|---|---|
1847 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}q_{2}$ | 0.6657 | 0.832 | 0.8002 | [M:[1.1198, 0.7298, 0.8802, 0.8802, 0.6797], q:[0.805, 0.5153], qb:[0.3649, 0.7549], phi:[0.39]] | t^2.039 + t^2.189 + t^2.34 + 2*t^2.641 + t^3.359 + t^3.51 + t^3.811 + t^4.078 + t^4.228 + t^4.262 + 2*t^4.379 + 2*t^4.529 + 4*t^4.68 + t^4.83 + 3*t^4.98 + 2*t^5.281 + t^5.398 + t^5.549 + 3*t^5.699 + t^5.85 - t^6. - t^4.17/y - t^4.17*y | detail |