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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1461 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6973 | 0.8507 | 0.8196 | [M:[1.03, 0.9101, 0.9401, 1.0, 1.0, 1.0599, 1.03], q:[0.515, 0.4551], qb:[0.5449, 0.5449], phi:[0.485]] | [M:[[2, 2], [-6, -6], [-7, -1], [3, -3], [-3, 3], [7, 1], [2, 2]], q:[[1, 1], [-3, -3]], qb:[[6, 0], [0, 6]], phi:[[-1, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{1}$, ${ }M_{7}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{7}$ | ${}M_{4}^{2}$, ${ }M_{5}^{2}$ | -3 | t^2.73 + 2*t^3. + 2*t^3.09 + 2*t^3.18 + t^4.185 + t^4.365 + 2*t^4.455 + t^4.545 + 2*t^4.635 + 3*t^4.725 + t^5.461 + t^5.82 - 3*t^6. + 2*t^6.09 + 5*t^6.18 + 2*t^6.27 + 3*t^6.359 + t^6.916 + t^7.096 + 2*t^7.185 + t^7.275 + 2*t^7.365 + 2*t^7.455 + 2*t^7.545 + 3*t^7.635 + 6*t^7.725 + 6*t^7.815 + 4*t^7.904 + t^8.191 + t^8.371 + 2*t^8.551 + 2*t^8.641 - 3*t^8.73 + 3*t^8.91 - t^4.455/y - t^7.185/y + t^7.365/y - t^7.545/y + t^7.725/y + (2*t^8.73)/y + (2*t^8.82)/y + (2*t^8.91)/y - t^4.455*y - t^7.185*y + t^7.365*y - t^7.545*y + t^7.725*y + 2*t^8.73*y + 2*t^8.82*y + 2*t^8.91*y | t^2.73/(g1^6*g2^6) + (g1^3*t^3.)/g2^3 + (g2^3*t^3.)/g1^3 + 2*g1^2*g2^2*t^3.09 + g1^7*g2*t^3.18 + g1*g2^7*t^3.18 + t^4.185/(g1^7*g2^7) + t^4.365/(g1^3*g2^3) + (g1^2*t^4.455)/g2^4 + (g2^2*t^4.455)/g1^4 + g1*g2*t^4.545 + g1^6*t^4.635 + g2^6*t^4.635 + (g1^11*t^4.725)/g2 + g1^5*g2^5*t^4.725 + (g2^11*t^4.725)/g1 + t^5.461/(g1^12*g2^12) + t^5.82/(g1^4*g2^4) - 3*t^6. + (g1^5*t^6.09)/g2 + (g2^5*t^6.09)/g1 + (g1^10*t^6.18)/g2^2 + 3*g1^4*g2^4*t^6.18 + (g2^10*t^6.18)/g1^2 + g1^9*g2^3*t^6.27 + g1^3*g2^9*t^6.27 + g1^14*g2^2*t^6.359 + g1^8*g2^8*t^6.359 + g1^2*g2^14*t^6.359 + t^6.916/(g1^13*g2^13) + t^7.096/(g1^9*g2^9) + t^7.185/(g1^4*g2^10) + t^7.185/(g1^10*g2^4) + t^7.275/(g1^5*g2^5) + t^7.365/g1^6 + t^7.365/g2^6 + (g1^5*t^7.455)/g2^7 + (g2^5*t^7.455)/g1^7 + (g1^4*t^7.545)/g2^2 + (g2^4*t^7.545)/g1^2 + (g1^9*t^7.635)/g2^3 + g1^3*g2^3*t^7.635 + (g2^9*t^7.635)/g1^3 + (g1^14*t^7.725)/g2^4 + 2*g1^8*g2^2*t^7.725 + 2*g1^2*g2^8*t^7.725 + (g2^14*t^7.725)/g1^4 + 2*g1^13*g2*t^7.815 + 2*g1^7*g2^7*t^7.815 + 2*g1*g2^13*t^7.815 + g1^18*t^7.904 + g1^12*g2^6*t^7.904 + g1^6*g2^12*t^7.904 + g2^18*t^7.904 + t^8.191/(g1^18*g2^18) + t^8.371/(g1^14*g2^14) + (2*t^8.551)/(g1^10*g2^10) + t^8.641/(g1^5*g2^11) + t^8.641/(g1^11*g2^5) - (3*t^8.73)/(g1^6*g2^6) + (g1^4*t^8.91)/g2^8 + t^8.91/(g1^2*g2^2) + (g2^4*t^8.91)/g1^8 - t^4.455/(g1*g2*y) - t^7.185/(g1^7*g2^7*y) + t^7.365/(g1^3*g2^3*y) - (g1*g2*t^7.545)/y + (g1^5*g2^5*t^7.725)/y + t^8.73/(g1^3*g2^9*y) + t^8.73/(g1^9*g2^3*y) + (2*t^8.82)/(g1^4*g2^4*y) + (g1*t^8.91)/(g2^5*y) + (g2*t^8.91)/(g1^5*y) - (t^4.455*y)/(g1*g2) - (t^7.185*y)/(g1^7*g2^7) + (t^7.365*y)/(g1^3*g2^3) - g1*g2*t^7.545*y + g1^5*g2^5*t^7.725*y + (t^8.73*y)/(g1^3*g2^9) + (t^8.73*y)/(g1^9*g2^3) + (2*t^8.82*y)/(g1^4*g2^4) + (g1*t^8.91*y)/g2^5 + (g2*t^8.91*y)/g1^5 |
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 |
---|---|---|---|---|---|---|---|---|---|
949 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ | 0.7004 | 0.8555 | 0.8187 | [M:[1.0368, 0.8895, 0.9263, 1.0, 1.0, 1.0737], q:[0.5184, 0.4448], qb:[0.5552, 0.5552], phi:[0.4816]] | t^2.669 + t^2.89 + 2*t^3. + t^3.11 + 2*t^3.221 + t^4.113 + t^4.334 + 2*t^4.445 + t^4.555 + 2*t^4.666 + 3*t^4.776 + t^5.337 + t^5.558 + t^5.779 + 2*t^5.89 - 2*t^6. - t^4.445/y - t^4.445*y | detail |