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 |
---|---|---|---|---|---|---|---|---|---|
1000 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ | 0.6946 | 0.8505 | 0.8168 | [M:[0.9879, 0.985, 1.0136, 0.9592, 1.0408, 0.9864], q:[0.5197, 0.4925], qb:[0.4668, 0.5483], phi:[0.4932]] | [M:[[16, 8], [-12, -12], [-2, 2], [6, -6], [-6, 6], [2, -2]], q:[[-10, -2], [-6, -6]], qb:[[12, 0], [0, 12]], phi:[[1, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{4}$, ${ }M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}^{2}$ | ${}$ | -3 | t^2.878 + t^2.955 + 2*t^2.959 + t^2.964 + t^3.122 + t^3.204 + t^4.28 + t^4.357 + t^4.434 + t^4.439 + t^4.516 + t^4.525 + t^4.598 + t^4.602 + t^4.683 + t^4.769 + 2*t^5.837 + t^5.91 + t^5.914 + 3*t^5.918 + t^5.923 + t^5.927 - 3*t^6. + t^6.082 + 2*t^6.163 + t^6.326 + t^6.408 + t^7.158 + t^7.235 + 2*t^7.239 + t^7.244 + t^7.312 + 2*t^7.317 - t^7.321 + t^7.389 + 2*t^7.394 + t^7.398 + t^7.402 + t^7.471 + t^7.475 - t^7.48 + 2*t^7.484 + t^7.488 + t^7.552 + 2*t^7.557 + 2*t^7.561 - t^7.566 + t^7.643 + t^7.647 + t^7.72 + 2*t^7.729 + t^7.733 + t^7.801 + t^7.806 - t^7.81 + t^7.887 + t^7.892 + t^7.973 + t^8.56 + t^8.637 + t^8.715 + t^8.792 + 3*t^8.796 - t^8.801 + t^8.805 + t^8.865 + 2*t^8.869 + 2*t^8.873 + t^8.878 + 3*t^8.882 + t^8.886 + t^8.891 + t^8.95 - 3*t^8.955 - 6*t^8.959 - 2*t^8.964 - t^4.48/y - t^7.434/y - t^7.439/y - t^7.443/y + t^7.516/y + t^7.52/y + t^7.525/y + t^8.833/y + (2*t^8.837)/y + t^8.841/y + (2*t^8.914)/y + (2*t^8.918)/y + (2*t^8.923)/y - t^4.48*y - t^7.434*y - t^7.439*y - t^7.443*y + t^7.516*y + t^7.52*y + t^7.525*y + t^8.833*y + 2*t^8.837*y + t^8.841*y + 2*t^8.914*y + 2*t^8.918*y + 2*t^8.923*y | (g1^6*t^2.878)/g2^6 + t^2.955/(g1^12*g2^12) + (2*g1^2*t^2.959)/g2^2 + g1^16*g2^8*t^2.964 + (g2^6*t^3.122)/g1^6 + (g2^10*t^3.204)/g1^10 + (g1^25*t^4.28)/g2 + (g1^7*t^4.357)/g2^7 + t^4.434/(g1^11*g2^13) + (g1^3*t^4.439)/g2^3 + t^4.516/(g1^15*g2^9) + g1^13*g2^11*t^4.525 + t^4.598/(g1^19*g2^5) + (g2^5*t^4.602)/g1^5 + (g2^9*t^4.683)/g1^9 + g1*g2^23*t^4.769 + (2*g1^8*t^5.837)/g2^8 + t^5.91/(g1^24*g2^24) + t^5.914/(g1^10*g2^14) + (3*g1^4*t^5.918)/g2^4 + g1^18*g2^6*t^5.923 + g1^32*g2^16*t^5.927 - 3*t^6. + (g2^4*t^6.082)/g1^4 + (2*g2^8*t^6.163)/g1^8 + (g2^16*t^6.326)/g1^16 + (g2^20*t^6.408)/g1^20 + (g1^31*t^7.158)/g2^7 + (g1^13*t^7.235)/g2^13 + (2*g1^27*t^7.239)/g2^3 + g1^41*g2^7*t^7.244 + t^7.312/(g1^5*g2^19) + (2*g1^9*t^7.317)/g2^9 - g1^23*g2*t^7.321 + t^7.389/(g1^23*g2^25) + (2*t^7.394)/(g1^9*g2^15) + (g1^5*t^7.398)/g2^5 + g1^19*g2^5*t^7.402 + t^7.471/(g1^27*g2^21) + t^7.475/(g1^13*g2^11) - (g1*t^7.48)/g2 + 2*g1^15*g2^9*t^7.484 + g1^29*g2^19*t^7.488 + t^7.552/(g1^31*g2^17) + (2*t^7.557)/(g1^17*g2^7) + (2*g2^3*t^7.561)/g1^3 - g1^11*g2^13*t^7.566 + (g2^7*t^7.643)/g1^7 + g1^7*g2^17*t^7.647 + (g2*t^7.72)/g1^25 + 2*g1^3*g2^21*t^7.729 + g1^17*g2^31*t^7.733 + (g2^5*t^7.801)/g1^29 + (g2^15*t^7.806)/g1^15 - (g2^25*t^7.81)/g1 + (g2^19*t^7.887)/g1^19 + (g2^29*t^7.892)/g1^5 + (g2^33*t^7.973)/g1^9 + (g1^50*t^8.56)/g2^2 + (g1^32*t^8.637)/g2^8 + (g1^14*t^8.715)/g2^14 + t^8.792/(g1^4*g2^20) + (3*g1^10*t^8.796)/g2^10 - g1^24*t^8.801 + g1^38*g2^10*t^8.805 + t^8.865/(g1^36*g2^36) + (2*t^8.869)/(g1^22*g2^26) + (2*t^8.873)/(g1^8*g2^16) + (g1^6*t^8.878)/g2^6 + 3*g1^20*g2^4*t^8.882 + g1^34*g2^14*t^8.886 + g1^48*g2^24*t^8.891 + t^8.95/(g1^26*g2^22) - (3*t^8.955)/(g1^12*g2^12) - (6*g1^2*t^8.959)/g2^2 - 2*g1^16*g2^8*t^8.964 - (g1*t^4.48)/(g2*y) - t^7.434/(g1^11*g2^13*y) - (g1^3*t^7.439)/(g2^3*y) - (g1^17*g2^7*t^7.443)/y + t^7.516/(g1^15*g2^9*y) + (g2*t^7.52)/(g1*y) + (g1^13*g2^11*t^7.525)/y + t^8.833/(g1^6*g2^18*y) + (2*g1^8*t^8.837)/(g2^8*y) + (g1^22*g2^2*t^8.841)/y + (2*t^8.914)/(g1^10*g2^14*y) + (2*g1^4*t^8.918)/(g2^4*y) + (2*g1^18*g2^6*t^8.923)/y - (g1*t^4.48*y)/g2 - (t^7.434*y)/(g1^11*g2^13) - (g1^3*t^7.439*y)/g2^3 - g1^17*g2^7*t^7.443*y + (t^7.516*y)/(g1^15*g2^9) + (g2*t^7.52*y)/g1 + g1^13*g2^11*t^7.525*y + (t^8.833*y)/(g1^6*g2^18) + (2*g1^8*t^8.837*y)/g2^8 + g1^22*g2^2*t^8.841*y + (2*t^8.914*y)/(g1^10*g2^14) + (2*g1^4*t^8.918*y)/g2^4 + 2*g1^18*g2^6*t^8.923*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 |
---|---|---|---|---|---|---|---|---|---|
612 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{3}\phi_{1}^{2}$ | 0.6935 | 0.8487 | 0.8171 | [M:[0.99, 0.9882, 1.0109, 0.9673, 1.0327], q:[0.5159, 0.4941], qb:[0.4732, 0.5386], phi:[0.4946]] | t^2.902 + t^2.964 + t^2.967 + t^2.97 + t^3.033 + t^3.098 + t^3.163 + t^4.323 + t^4.386 + t^4.448 + t^4.451 + t^4.514 + t^4.519 + t^4.579 + t^4.582 + t^4.647 + t^4.715 + t^5.869 + t^5.929 + 2*t^5.935 + t^5.94 + t^5.997 - 2*t^6. - t^4.484/y - t^4.484*y | detail |