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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3247 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.6291 | 0.8166 | 0.7704 | [M:[1.0, 1.0425, 0.915, 0.7181, 0.7181], q:[0.7606, 0.2394], qb:[0.5213, 0.5638], phi:[0.4787]] | [M:[[0], [4], [-8], [-3], [-3]], q:[[1], [-1]], qb:[[2], [6]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}^{2}q_{2}^{4}$, ${ }M_{2}M_{3}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ | ${}\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$ | -1 | 2*t^2.154 + t^2.282 + t^2.409 + t^2.745 + t^2.872 + t^3. + t^3.128 + t^3.718 + t^3.973 + 3*t^4.309 + 2*t^4.436 + 4*t^4.564 + 2*t^4.691 + 2*t^4.819 + 2*t^4.899 + 2*t^5.027 + 3*t^5.154 + 4*t^5.282 + 2*t^5.409 + t^5.49 + t^5.537 + t^5.617 + 2*t^5.745 + 2*t^5.872 - t^6. + 2*t^6.128 + t^6.255 + t^6.383 + 4*t^6.463 + 2*t^6.591 + 6*t^6.718 + 4*t^6.846 + 5*t^6.973 + 3*t^7.054 + 3*t^7.101 + 3*t^7.181 + 2*t^7.228 + 5*t^7.309 + 7*t^7.436 + 4*t^7.564 + 2*t^7.644 + 5*t^7.691 + 2*t^7.772 + 2*t^7.819 + 4*t^7.899 + 2*t^7.946 + 4*t^8.027 - 2*t^8.154 + t^8.235 + t^8.282 + t^8.362 - 2*t^8.409 + 2*t^8.49 + 2*t^8.537 + 7*t^8.617 + t^8.665 + 2*t^8.792 + 5*t^8.872 - t^4.436/y - (2*t^6.591)/y - t^7.181/y + t^7.309/y + (2*t^7.436)/y + (2*t^7.564)/y + (2*t^7.691)/y + (2*t^7.899)/y + (3*t^8.027)/y + (4*t^8.154)/y + (6*t^8.282)/y + (2*t^8.409)/y + t^8.537/y + t^8.617/y - (2*t^8.745)/y + (4*t^8.872)/y - t^4.436*y - 2*t^6.591*y - t^7.181*y + t^7.309*y + 2*t^7.436*y + 2*t^7.564*y + 2*t^7.691*y + 2*t^7.899*y + 3*t^8.027*y + 4*t^8.154*y + 6*t^8.282*y + 2*t^8.409*y + t^8.537*y + t^8.617*y - 2*t^8.745*y + 4*t^8.872*y | (2*t^2.154)/g1^3 + g1*t^2.282 + g1^5*t^2.409 + t^2.745/g1^8 + t^2.872/g1^4 + t^3. + g1^4*t^3.128 + t^3.718/g1 + g1^7*t^3.973 + (3*t^4.309)/g1^6 + (2*t^4.436)/g1^2 + 4*g1^2*t^4.564 + 2*g1^6*t^4.691 + 2*g1^10*t^4.819 + (2*t^4.899)/g1^11 + (2*t^5.027)/g1^7 + (3*t^5.154)/g1^3 + 4*g1*t^5.282 + 2*g1^5*t^5.409 + t^5.49/g1^16 + g1^9*t^5.537 + t^5.617/g1^12 + (2*t^5.745)/g1^8 + (2*t^5.872)/g1^4 - t^6. + 2*g1^4*t^6.128 + g1^8*t^6.255 + g1^12*t^6.383 + (4*t^6.463)/g1^9 + (2*t^6.591)/g1^5 + (6*t^6.718)/g1 + 4*g1^3*t^6.846 + 5*g1^7*t^6.973 + (3*t^7.054)/g1^14 + 3*g1^11*t^7.101 + (3*t^7.181)/g1^10 + 2*g1^15*t^7.228 + (5*t^7.309)/g1^6 + (7*t^7.436)/g1^2 + 4*g1^2*t^7.564 + (2*t^7.644)/g1^19 + 5*g1^6*t^7.691 + (2*t^7.772)/g1^15 + 2*g1^10*t^7.819 + (4*t^7.899)/g1^11 + 2*g1^14*t^7.946 + (4*t^8.027)/g1^7 - (2*t^8.154)/g1^3 + t^8.235/g1^24 + g1*t^8.282 + t^8.362/g1^20 - 2*g1^5*t^8.409 + (2*t^8.49)/g1^16 + 2*g1^9*t^8.537 + (7*t^8.617)/g1^12 + g1^13*t^8.665 + 2*g1^17*t^8.792 + (5*t^8.872)/g1^4 - t^4.436/(g1^2*y) - (2*t^6.591)/(g1^5*y) - t^7.181/(g1^10*y) + t^7.309/(g1^6*y) + (2*t^7.436)/(g1^2*y) + (2*g1^2*t^7.564)/y + (2*g1^6*t^7.691)/y + (2*t^7.899)/(g1^11*y) + (3*t^8.027)/(g1^7*y) + (4*t^8.154)/(g1^3*y) + (6*g1*t^8.282)/y + (2*g1^5*t^8.409)/y + (g1^9*t^8.537)/y + t^8.617/(g1^12*y) - (2*t^8.745)/(g1^8*y) + (4*t^8.872)/(g1^4*y) - (t^4.436*y)/g1^2 - (2*t^6.591*y)/g1^5 - (t^7.181*y)/g1^10 + (t^7.309*y)/g1^6 + (2*t^7.436*y)/g1^2 + 2*g1^2*t^7.564*y + 2*g1^6*t^7.691*y + (2*t^7.899*y)/g1^11 + (3*t^8.027*y)/g1^7 + (4*t^8.154*y)/g1^3 + 6*g1*t^8.282*y + 2*g1^5*t^8.409*y + g1^9*t^8.537*y + (t^8.617*y)/g1^12 - (2*t^8.745*y)/g1^8 + (4*t^8.872*y)/g1^4 |
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 |
---|---|---|---|---|---|---|---|---|---|
2734 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.609 | 0.779 | 0.7817 | [M:[1.0, 1.0388, 0.9224, 0.7209], q:[0.7597, 0.2403], qb:[0.5194, 0.5582], phi:[0.4806]] | t^2.163 + t^2.279 + t^2.395 + t^2.767 + t^2.884 + t^3. + t^3.116 + t^3.721 + t^3.837 + t^3.954 + t^4.325 + t^4.442 + 3*t^4.558 + 2*t^4.675 + 2*t^4.791 + t^4.93 + t^5.046 + 2*t^5.163 + 3*t^5.279 + 2*t^5.395 + t^5.512 + t^5.535 + t^5.651 + 2*t^5.767 + t^5.884 - t^4.442/y - t^4.442*y | detail |