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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55381 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ | 0.6676 | 0.842 | 0.7928 | [M:[0.8363, 1.2091, 0.7909, 0.7455, 0.8363, 0.8818], q:[0.7455, 0.4182], qb:[0.3727, 0.7909], phi:[0.4182]] | [M:[[-4], [-1], [1], [6], [-4], [-9]], q:[[6], [-2]], qb:[[3], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{4}$, ${ }M_{3}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{3}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ | 1 | t^2.236 + t^2.373 + 3*t^2.509 + t^2.645 + t^3.491 + 2*t^3.627 + t^4.473 + 3*t^4.609 + 5*t^4.745 + 3*t^4.882 + 6*t^5.018 + 3*t^5.154 + t^5.291 + 2*t^5.727 + 2*t^5.864 + t^6. + 3*t^6.136 + t^6.273 + t^6.709 + 3*t^6.846 + 4*t^6.982 + 6*t^7.118 + 10*t^7.255 + 6*t^7.391 + 11*t^7.527 + 6*t^7.663 + 3*t^7.8 + t^7.936 + 2*t^7.964 + 2*t^8.1 + 3*t^8.236 - t^8.373 - 3*t^8.509 + t^8.645 + t^8.918 + t^8.946 - t^4.255/y - t^6.491/y - (3*t^6.764)/y - t^6.9/y + (2*t^7.609)/y + (6*t^7.745)/y + (4*t^7.882)/y + (5*t^8.018)/y + (3*t^8.154)/y + (3*t^8.864)/y - t^4.255*y - t^6.491*y - 3*t^6.764*y - t^6.9*y + 2*t^7.609*y + 6*t^7.745*y + 4*t^7.882*y + 5*t^8.018*y + 3*t^8.154*y + 3*t^8.864*y | g1^6*t^2.236 + g1*t^2.373 + (3*t^2.509)/g1^4 + t^2.645/g1^9 + g1^4*t^3.491 + (2*t^3.627)/g1 + g1^12*t^4.473 + 3*g1^7*t^4.609 + 5*g1^2*t^4.745 + (3*t^4.882)/g1^3 + (6*t^5.018)/g1^8 + (3*t^5.154)/g1^13 + t^5.291/g1^18 + 2*g1^10*t^5.727 + 2*g1^5*t^5.864 + t^6. + (3*t^6.136)/g1^5 + t^6.273/g1^10 + g1^18*t^6.709 + 3*g1^13*t^6.846 + 4*g1^8*t^6.982 + 6*g1^3*t^7.118 + (10*t^7.255)/g1^2 + (6*t^7.391)/g1^7 + (11*t^7.527)/g1^12 + (6*t^7.663)/g1^17 + (3*t^7.8)/g1^22 + t^7.936/g1^27 + 2*g1^16*t^7.964 + 2*g1^11*t^8.1 + 3*g1^6*t^8.236 - g1*t^8.373 - (3*t^8.509)/g1^4 + t^8.645/g1^9 + t^8.918/g1^19 + g1^24*t^8.946 - t^4.255/(g1^2*y) - (g1^4*t^6.491)/y - (3*t^6.764)/(g1^6*y) - t^6.9/(g1^11*y) + (2*g1^7*t^7.609)/y + (6*g1^2*t^7.745)/y + (4*t^7.882)/(g1^3*y) + (5*t^8.018)/(g1^8*y) + (3*t^8.154)/(g1^13*y) + (3*g1^5*t^8.864)/y - (t^4.255*y)/g1^2 - g1^4*t^6.491*y - (3*t^6.764*y)/g1^6 - (t^6.9*y)/g1^11 + 2*g1^7*t^7.609*y + 6*g1^2*t^7.745*y + (4*t^7.882*y)/g1^3 + (5*t^8.018*y)/g1^8 + (3*t^8.154*y)/g1^13 + 3*g1^5*t^8.864*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 |
---|---|---|---|---|---|---|---|---|---|
46951 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ | 0.6598 | 0.8306 | 0.7944 | [M:[0.8664, 1.2166, 0.7834, 0.7003, 0.8664], q:[0.7003, 0.4332], qb:[0.3502, 0.7834], phi:[0.4332]] | t^2.101 + t^2.35 + 3*t^2.599 + t^3.151 + t^3.401 + 2*t^3.65 + t^4.202 + 3*t^4.451 + 5*t^4.7 + 2*t^4.95 + 5*t^5.199 + t^5.252 + 3*t^5.502 + 5*t^5.751 + t^6. - t^4.3/y - t^4.3*y | detail |