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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56235 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6959 | 0.9008 | 0.7725 | [M:[0.7628, 1.1442, 0.8558, 0.6699, 0.6699, 0.7628, 0.7628], q:[0.8558, 0.3814], qb:[0.4744, 0.7628], phi:[0.3814]] | [M:[[2], [3], [-3], [7], [7], [2], [2]], q:[[-3], [1]], qb:[[-4], [2]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{4}$, ${ }M_{5}$, ${ }M_{1}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | ${}M_{3}\phi_{1}q_{2}^{2}$ | -3 | 2*t^2.01 + 4*t^2.288 + t^2.567 + 2*t^3.433 + 3*t^4.019 + 8*t^4.298 + 12*t^4.577 + 5*t^4.856 + t^5.135 + 4*t^5.442 + 6*t^5.721 - 3*t^6. + 4*t^6.029 - 2*t^6.279 + 12*t^6.308 + 23*t^6.586 + 31*t^6.865 + 10*t^7.144 - 2*t^7.423 + 6*t^7.452 - t^7.702 + 12*t^7.731 + 6*t^8.01 + 5*t^8.038 - 17*t^8.288 + 16*t^8.317 - 15*t^8.567 + 34*t^8.596 - 4*t^8.846 + 57*t^8.875 - t^4.144/y - (2*t^6.154)/y - (4*t^6.433)/y + t^7.019/y + (8*t^7.298)/y + (8*t^7.577)/y + (8*t^7.856)/y + (2*t^8.135)/y - (3*t^8.163)/y - (4*t^8.442)/y - (2*t^8.721)/y - t^4.144*y - 2*t^6.154*y - 4*t^6.433*y + t^7.019*y + 8*t^7.298*y + 8*t^7.577*y + 8*t^7.856*y + 2*t^8.135*y - 3*t^8.163*y - 4*t^8.442*y - 2*t^8.721*y | 2*g1^7*t^2.01 + 4*g1^2*t^2.288 + t^2.567/g1^3 + 2*g1^3*t^3.433 + 3*g1^14*t^4.019 + 8*g1^9*t^4.298 + 12*g1^4*t^4.577 + (5*t^4.856)/g1 + t^5.135/g1^6 + 4*g1^10*t^5.442 + 6*g1^5*t^5.721 - 3*t^6. + 4*g1^21*t^6.029 - (2*t^6.279)/g1^5 + 12*g1^16*t^6.308 + 23*g1^11*t^6.586 + 31*g1^6*t^6.865 + 10*g1*t^7.144 - (2*t^7.423)/g1^4 + 6*g1^17*t^7.452 - t^7.702/g1^9 + 12*g1^12*t^7.731 + 6*g1^7*t^8.01 + 5*g1^28*t^8.038 - 17*g1^2*t^8.288 + 16*g1^23*t^8.317 - (15*t^8.567)/g1^3 + 34*g1^18*t^8.596 - (4*t^8.846)/g1^8 + 57*g1^13*t^8.875 - (g1*t^4.144)/y - (2*g1^8*t^6.154)/y - (4*g1^3*t^6.433)/y + (g1^14*t^7.019)/y + (8*g1^9*t^7.298)/y + (8*g1^4*t^7.577)/y + (8*t^7.856)/(g1*y) + (2*t^8.135)/(g1^6*y) - (3*g1^15*t^8.163)/y - (4*g1^10*t^8.442)/y - (2*g1^5*t^8.721)/y - g1*t^4.144*y - 2*g1^8*t^6.154*y - 4*g1^3*t^6.433*y + g1^14*t^7.019*y + 8*g1^9*t^7.298*y + 8*g1^4*t^7.577*y + (8*t^7.856*y)/g1 + (2*t^8.135*y)/g1^6 - 3*g1^15*t^8.163*y - 4*g1^10*t^8.442*y - 2*g1^5*t^8.721*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 |
---|---|---|---|---|---|---|---|---|---|
51268 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6775 | 0.8668 | 0.7816 | [M:[0.7647, 1.147, 0.853, 0.6764, 0.6764, 0.7647], q:[0.853, 0.3823], qb:[0.4706, 0.7647], phi:[0.3823]] | 2*t^2.029 + 3*t^2.294 + t^2.559 + 2*t^3.441 + t^3.706 + 3*t^4.059 + 6*t^4.323 + 8*t^4.588 + 4*t^4.853 + t^5.118 + 4*t^5.47 + 6*t^5.735 - t^4.147/y - t^4.147*y | detail |