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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# | 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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422 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ | 0.6786 | 0.8339 | 0.8138 | [M:[0.9772, 1.1268, 0.9523, 0.7692, 0.8732], q:[0.7817, 0.4242], qb:[0.5987, 0.4491], phi:[0.4366]] | [M:[[-7, 1], [4, 0], [-11, -1], [-1, -1], [-4, 0]], q:[[1, 0], [-4, -1]], qb:[[11, 0], [0, 1]], phi:[[-2, 0]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{4}$, ${ }M_{5}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}^{2}$ | ${}$ | -3 | t^2.308 + 2*t^2.62 + t^2.857 + t^2.932 + t^3.618 + t^3.855 + t^3.929 + t^4.004 + t^4.141 + t^4.378 + t^4.453 + t^4.615 + t^4.902 + 2*t^4.927 + t^5.165 + 4*t^5.239 + t^5.477 + t^5.551 + t^5.714 + t^5.788 + t^5.863 - 3*t^6. - t^6.075 + t^6.163 + 2*t^6.237 + 3*t^6.474 - t^6.523 + 2*t^6.549 + 2*t^6.624 + t^6.686 + t^6.712 + t^6.761 + t^6.786 + t^6.861 + t^6.923 + t^6.936 + t^6.998 + t^7.073 + t^7.209 + 2*t^7.235 - t^7.31 - t^7.385 + 2*t^7.472 + t^7.521 + 4*t^7.547 + t^7.71 + 2*t^7.784 - t^7.833 + 6*t^7.859 + t^7.934 + t^7.996 + t^8.008 + t^8.021 + 2*t^8.096 + 2*t^8.171 + t^8.233 - 3*t^8.308 + t^8.333 - t^8.382 + t^8.408 + t^8.457 + t^8.47 + t^8.483 + t^8.519 + t^8.571 - 6*t^8.62 + t^8.645 - 2*t^8.694 + t^8.72 + t^8.757 + 2*t^8.782 + t^8.795 - t^8.831 + t^8.906 - 3*t^8.932 + t^8.994 - t^4.31/y - t^6.618/y - t^6.929/y - t^7.167/y - t^7.241/y + t^7.378/y + t^7.453/y + t^7.69/y + (2*t^7.927)/y + t^8.002/y + t^8.165/y + (2*t^8.239)/y + (2*t^8.477)/y + (2*t^8.551)/y + t^8.788/y - t^4.31*y - t^6.618*y - t^6.929*y - t^7.167*y - t^7.241*y + t^7.378*y + t^7.453*y + t^7.69*y + 2*t^7.927*y + t^8.002*y + t^8.165*y + 2*t^8.239*y + 2*t^8.477*y + 2*t^8.551*y + t^8.788*y | t^2.308/(g1*g2) + (2*t^2.62)/g1^4 + t^2.857/(g1^11*g2) + (g2*t^2.932)/g1^7 + t^3.618/(g1^3*g2) + t^3.855/(g1^10*g2^2) + t^3.929/g1^6 + (g2^2*t^4.004)/g1^2 + g1^12*t^4.141 + (g1^5*t^4.378)/g2 + g1^9*g2*t^4.453 + t^4.615/(g1^2*g2^2) + g1^20*t^4.902 + (2*t^4.927)/(g1^5*g2) + t^5.165/(g1^12*g2^2) + (4*t^5.239)/g1^8 + t^5.477/(g1^15*g2) + (g2*t^5.551)/g1^11 + t^5.714/(g1^22*g2^2) + t^5.788/g1^18 + (g2^2*t^5.863)/g1^14 - 3*t^6. - g1^4*g2^2*t^6.075 + t^6.163/(g1^11*g2^3) + (2*t^6.237)/(g1^7*g2) + (3*t^6.474)/(g1^14*g2^2) - g1^15*g2*t^6.523 + (2*t^6.549)/g1^10 + (2*g2^2*t^6.624)/g1^6 + (g1^4*t^6.686)/g2^2 + t^6.712/(g1^21*g2^3) + g1^8*t^6.761 + t^6.786/(g1^17*g2) + (g2*t^6.861)/g1^13 + t^6.923/(g1^3*g2^3) + (g2^3*t^6.936)/g1^9 + (g1*t^6.998)/g2 + g1^5*g2*t^7.073 + (g1^19*t^7.209)/g2 + (2*t^7.235)/(g1^6*g2^2) - t^7.31/g1^2 - g1^2*g2^2*t^7.385 + (2*t^7.472)/(g1^13*g2^3) + g1^16*t^7.521 + (4*t^7.547)/(g1^9*g2) + t^7.71/(g1^20*g2^4) + (2*t^7.784)/(g1^16*g2^2) - g1^13*g2*t^7.833 + (6*t^7.859)/g1^12 + (g2^2*t^7.934)/g1^8 + (g1^2*t^7.996)/g2^2 + (g2^4*t^8.008)/g1^4 + t^8.021/(g1^23*g2^3) + (2*t^8.096)/(g1^19*g2) + (2*g2*t^8.171)/g1^15 + t^8.233/(g1^5*g2^3) - (3*t^8.308)/(g1*g2) + t^8.333/(g1^26*g2^2) - g1^3*g2*t^8.382 + t^8.408/g1^22 + g1^7*g2^3*t^8.457 + t^8.47/(g1^12*g2^4) + (g2^2*t^8.483)/g1^18 + (g1^17*t^8.519)/g2 + t^8.571/(g1^33*g2^3) - (6*t^8.62)/g1^4 + t^8.645/(g1^29*g2) - 2*g2^2*t^8.694 + (g2*t^8.72)/g1^25 + (g1^10*t^8.757)/g2^2 + (2*t^8.782)/(g1^15*g2^3) + (g2^3*t^8.795)/g1^21 - g1^14*t^8.831 + g1^18*g2^2*t^8.906 - (3*g2*t^8.932)/g1^7 + (g1^3*t^8.994)/g2^3 - t^4.31/(g1^2*y) - t^6.618/(g1^3*g2*y) - t^6.929/(g1^6*y) - t^7.167/(g1^13*g2*y) - (g2*t^7.241)/(g1^9*y) + (g1^5*t^7.378)/(g2*y) + (g1^9*g2*t^7.453)/y + (g1^2*t^7.69)/y + (2*t^7.927)/(g1^5*g2*y) + (g2*t^8.002)/(g1*y) + t^8.165/(g1^12*g2^2*y) + (2*t^8.239)/(g1^8*y) + (2*t^8.477)/(g1^15*g2*y) + (2*g2*t^8.551)/(g1^11*y) + t^8.788/(g1^18*y) - (t^4.31*y)/g1^2 - (t^6.618*y)/(g1^3*g2) - (t^6.929*y)/g1^6 - (t^7.167*y)/(g1^13*g2) - (g2*t^7.241*y)/g1^9 + (g1^5*t^7.378*y)/g2 + g1^9*g2*t^7.453*y + g1^2*t^7.69*y + (2*t^7.927*y)/(g1^5*g2) + (g2*t^8.002*y)/g1 + (t^8.165*y)/(g1^12*g2^2) + (2*t^8.239*y)/g1^8 + (2*t^8.477*y)/(g1^15*g2) + (2*g2*t^8.551*y)/g1^11 + (t^8.788*y)/g1^18 |
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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# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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699 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ | 0.6682 | 0.8218 | 0.813 | [M:[1.0917, 1.0917, 0.9959, 0.725, 0.9083], q:[0.7729, 0.4063], qb:[0.502, 0.502], phi:[0.4542]] | t^2.175 + 2*t^2.725 + t^2.988 + t^3.275 + t^3.538 + t^3.8 + t^3.825 + 2*t^4.088 + t^4.35 + 3*t^4.375 + 2*t^4.9 + t^5.163 + 4*t^5.45 + t^5.713 + 2*t^5.975 - 2*t^6. - t^4.363/y - t^4.363*y | detail | |
701 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{3}^{2}$ | 0.6768 | 0.8295 | 0.8159 | [M:[0.9891, 1.1135, 1.0, 0.7838, 0.8865], q:[0.7784, 0.4487], qb:[0.5622, 0.4378], phi:[0.4432]] | t^2.351 + 2*t^2.659 + t^2.967 + t^3. + t^3.681 + t^3.957 + t^3.989 + 2*t^4.022 + t^4.33 + t^4.362 + 2*t^4.703 + 2*t^5.011 + 4*t^5.319 + t^5.351 + t^5.627 + t^5.659 + t^5.935 - 2*t^6. - t^4.33/y - t^4.33*y | detail | |
705 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ | 0.699 | 0.8725 | 0.8011 | [M:[0.974, 1.1248, 0.9642, 0.7763, 0.8752, 0.697], q:[0.7812, 0.4327], qb:[0.5933, 0.4424], phi:[0.4376]] | t^2.091 + t^2.329 + 2*t^2.625 + t^2.893 + t^2.922 + t^3.642 + t^3.938 + t^3.967 + t^4.124 + t^4.182 + t^4.391 + 2*t^4.42 + t^4.658 + 2*t^4.716 + t^4.873 + 2*t^4.955 + t^4.984 + t^5.013 + t^5.222 + 4*t^5.251 + t^5.518 + t^5.547 + t^5.733 + t^5.785 + t^5.815 + t^5.844 - 3*t^6. - t^4.313/y - t^4.313*y | detail | |
706 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{6}q_{1}q_{2}$ | 0.6958 | 0.8638 | 0.8055 | [M:[0.9672, 1.1257, 0.9672, 0.7814, 0.8743, 0.7814], q:[0.7814, 0.4372], qb:[0.5957, 0.4372], phi:[0.4372]] | 2*t^2.344 + 2*t^2.623 + 2*t^2.902 + 3*t^3.934 + t^4.131 + 2*t^4.41 + 3*t^4.689 + t^4.885 + 4*t^4.967 + 7*t^5.246 + 2*t^5.524 + 3*t^5.803 - 5*t^6. - t^4.311/y - t^4.311*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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# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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No data available in table |
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 |
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# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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265 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ | 0.6675 | 0.8146 | 0.8195 | [M:[0.9917, 1.1204, 0.9667, 0.7676], q:[0.7801, 0.4273], qb:[0.581, 0.4523], phi:[0.4398]] | t^2.303 + t^2.639 + t^2.9 + t^2.975 + t^3.361 + t^3.622 + t^3.883 + t^3.958 + t^4.033 + t^4.083 + t^4.344 + t^4.419 + t^4.605 + t^4.805 + t^4.942 + t^5.203 + 2*t^5.278 + t^5.664 + t^5.8 + t^5.875 + t^5.95 - 2*t^6. - t^4.319/y - t^4.319*y | detail |