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 |
---|---|---|---|---|---|---|---|---|---|
46111 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ | 0.5532 | 0.705 | 0.7847 | [M:[0.857, 1.143, 0.7135], q:[1.0005, 0.571], qb:[0.286, 0.4285], phi:[0.4285]] | [M:[[2], [-2], [11]], q:[[-7], [6]], qb:[[-4], [1]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}M_{1}M_{2}$ | 0 | t^2.14 + t^2.144 + 2*t^2.571 + t^2.998 + t^3.002 + t^3.429 + t^3.856 + t^4.281 + t^4.284 + 2*t^4.287 + 2*t^4.711 + 3*t^4.715 + t^5.139 + 4*t^5.142 + t^5.145 + 2*t^5.569 + 2*t^5.573 + 2*t^5.997 + t^6.003 + t^6.421 + t^6.424 + 2*t^6.427 + t^6.431 + 2*t^6.852 + 3*t^6.855 + 2*t^6.858 + t^7.279 + 4*t^7.282 + 4*t^7.285 + t^7.289 + 2*t^7.71 + 5*t^7.713 + t^7.716 + 2*t^8.137 + t^8.14 + t^8.147 + t^8.562 + t^8.565 + 3*t^8.568 - 2*t^8.571 + 2*t^8.574 + 2*t^8.992 + 4*t^8.995 - t^8.998 - t^4.285/y - t^6.426/y - t^6.856/y + t^7.284/y + (2*t^7.711)/y + (3*t^7.715)/y + t^8.139/y + (3*t^8.142)/y + (2*t^8.145)/y - t^8.566/y + (3*t^8.569)/y + (3*t^8.573)/y - t^4.285*y - t^6.426*y - t^6.856*y + t^7.284*y + 2*t^7.711*y + 3*t^7.715*y + t^8.139*y + 3*t^8.142*y + 2*t^8.145*y - t^8.566*y + 3*t^8.569*y + 3*t^8.573*y | g1^11*t^2.14 + t^2.144/g1^3 + 2*g1^2*t^2.571 + g1^7*t^2.998 + t^3.002/g1^7 + t^3.429/g1^2 + g1^3*t^3.856 + g1^22*t^4.281 + g1^8*t^4.284 + (2*t^4.287)/g1^6 + 2*g1^13*t^4.711 + (3*t^4.715)/g1 + g1^18*t^5.139 + 4*g1^4*t^5.142 + t^5.145/g1^10 + 2*g1^9*t^5.569 + (2*t^5.573)/g1^5 + 2*g1^14*t^5.997 + t^6.003/g1^14 + g1^33*t^6.421 + g1^19*t^6.424 + 2*g1^5*t^6.427 + t^6.431/g1^9 + 2*g1^24*t^6.852 + 3*g1^10*t^6.855 + (2*t^6.858)/g1^4 + g1^29*t^7.279 + 4*g1^15*t^7.282 + 4*g1*t^7.285 + t^7.289/g1^13 + 2*g1^20*t^7.71 + 5*g1^6*t^7.713 + t^7.716/g1^8 + 2*g1^25*t^8.137 + g1^11*t^8.14 + t^8.147/g1^17 + g1^44*t^8.562 + g1^30*t^8.565 + 3*g1^16*t^8.568 - 2*g1^2*t^8.571 + (2*t^8.574)/g1^12 + 2*g1^35*t^8.992 + 4*g1^21*t^8.995 - g1^7*t^8.998 - (g1*t^4.285)/y - (g1^12*t^6.426)/y - (g1^3*t^6.856)/y + (g1^8*t^7.284)/y + (2*g1^13*t^7.711)/y + (3*t^7.715)/(g1*y) + (g1^18*t^8.139)/y + (3*g1^4*t^8.142)/y + (2*t^8.145)/(g1^10*y) - (g1^23*t^8.566)/y + (3*g1^9*t^8.569)/y + (3*t^8.573)/(g1^5*y) - g1*t^4.285*y - g1^12*t^6.426*y - g1^3*t^6.856*y + g1^8*t^7.284*y + 2*g1^13*t^7.711*y + (3*t^7.715*y)/g1 + g1^18*t^8.139*y + 3*g1^4*t^8.142*y + (2*t^8.145*y)/g1^10 - g1^23*t^8.566*y + 3*g1^9*t^8.569*y + (3*t^8.573*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 |
---|---|---|---|---|---|---|---|---|
46458 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ | 0.5546 | 0.7066 | 0.7848 | [M:[0.8656, 1.1344, 0.7611, 0.9702], q:[0.9702, 0.5969], qb:[0.2687, 0.4328], phi:[0.4328]] | t^2.105 + t^2.283 + 2*t^2.597 + 2*t^2.911 + t^3.403 + t^3.895 + 2*t^4.209 + t^4.388 + t^4.566 + 3*t^4.702 + 2*t^4.88 + 2*t^5.015 + 4*t^5.194 + 4*t^5.508 + 3*t^5.821 - t^6. - t^4.298/y - t^4.298*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
46028 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ | 0.5333 | 0.6681 | 0.7983 | [M:[0.8626, 1.1374], q:[0.981, 0.5878], qb:[0.2748, 0.4313], phi:[0.4313]] | t^2.118 + 2*t^2.588 + t^2.943 + t^3.057 + t^3.412 + t^3.767 + t^3.882 + 2*t^4.237 + 3*t^4.706 + t^5.061 + 3*t^5.176 + 2*t^5.531 + t^5.645 + 2*t^5.886 - t^4.294/y - t^4.294*y | detail |