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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55953 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}^{2}$ | 0.6726 | 0.8389 | 0.8018 | [M:[1.159, 1.046, 0.841, 0.7727, 0.7043, 1.0907], q:[0.3863, 0.4547], qb:[0.5676, 0.7727], phi:[0.4547]] | [M:[[3], [-18], [-3], [2], [7], [8]], q:[[1], [-4]], qb:[[17], [2]], phi:[[-4]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{5}$, ${ }M_{4}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{6}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{5}\phi_{1}q_{1}^{2}$ | ${}$ | -1 | t^2.113 + t^2.318 + t^2.523 + t^3.067 + t^3.138 + t^3.272 + t^3.477 + t^3.682 + t^4.021 + t^4.092 + 2*t^4.226 + 2*t^4.431 + 2*t^4.636 + t^4.77 + t^4.841 + t^5.046 + t^5.18 + t^5.251 + 2*t^5.385 + 3*t^5.59 + 2*t^5.795 - t^6. + 2*t^6.134 + t^6.205 + t^6.276 + 3*t^6.339 + t^6.41 + 4*t^6.544 + t^6.615 + 4*t^6.749 + t^6.883 + 2*t^6.954 - t^7.025 + 2*t^7.088 + 2*t^7.159 + t^7.23 + 3*t^7.293 + t^7.364 + 4*t^7.498 + t^7.569 + 4*t^7.703 + t^7.837 + 4*t^7.908 - t^7.979 + t^8.042 + t^8.184 + 3*t^8.247 - t^8.318 + t^8.389 + 5*t^8.452 - t^8.523 + t^8.594 + 5*t^8.657 + t^8.791 + 6*t^8.862 - t^8.933 + 2*t^8.996 - t^4.364/y - t^6.477/y - t^6.682/y + t^7.226/y + t^7.431/y - t^7.502/y + t^7.636/y + t^7.841/y + t^8.046/y + t^8.18/y + (2*t^8.251)/y + (2*t^8.385)/y + t^8.456/y + (2*t^8.59)/y + t^8.661/y + (2*t^8.795)/y - t^4.364*y - t^6.477*y - t^6.682*y + t^7.226*y + t^7.431*y - t^7.502*y + t^7.636*y + t^7.841*y + t^8.046*y + t^8.18*y + 2*t^8.251*y + 2*t^8.385*y + t^8.456*y + 2*t^8.59*y + t^8.661*y + 2*t^8.795*y | g1^7*t^2.113 + g1^2*t^2.318 + t^2.523/g1^3 + g1^13*t^3.067 + t^3.138/g1^18 + g1^8*t^3.272 + g1^3*t^3.477 + t^3.682/g1^2 + g1^19*t^4.021 + t^4.092/g1^12 + 2*g1^14*t^4.226 + 2*g1^9*t^4.431 + 2*g1^4*t^4.636 + g1^30*t^4.77 + t^4.841/g1 + t^5.046/g1^6 + g1^20*t^5.18 + t^5.251/g1^11 + 2*g1^15*t^5.385 + 3*g1^10*t^5.59 + 2*g1^5*t^5.795 - t^6. + 2*g1^26*t^6.134 + t^6.205/g1^5 + t^6.276/g1^36 + 3*g1^21*t^6.339 + t^6.41/g1^10 + 4*g1^16*t^6.544 + t^6.615/g1^15 + 4*g1^11*t^6.749 + g1^37*t^6.883 + 2*g1^6*t^6.954 - t^7.025/g1^25 + 2*g1^32*t^7.088 + 2*g1*t^7.159 + t^7.23/g1^30 + 3*g1^27*t^7.293 + t^7.364/g1^4 + 4*g1^22*t^7.498 + t^7.569/g1^9 + 4*g1^17*t^7.703 + g1^43*t^7.837 + 4*g1^12*t^7.908 - t^7.979/g1^19 + g1^38*t^8.042 + t^8.184/g1^24 + 3*g1^33*t^8.247 - g1^2*t^8.318 + t^8.389/g1^29 + 5*g1^28*t^8.452 - t^8.523/g1^3 + t^8.594/g1^34 + 5*g1^23*t^8.657 + g1^49*t^8.791 + 6*g1^18*t^8.862 - t^8.933/g1^13 + 2*g1^44*t^8.996 - t^4.364/(g1^4*y) - (g1^3*t^6.477)/y - t^6.682/(g1^2*y) + (g1^14*t^7.226)/y + (g1^9*t^7.431)/y - t^7.502/(g1^22*y) + (g1^4*t^7.636)/y + t^7.841/(g1*y) + t^8.046/(g1^6*y) + (g1^20*t^8.18)/y + (2*t^8.251)/(g1^11*y) + (2*g1^15*t^8.385)/y + t^8.456/(g1^16*y) + (2*g1^10*t^8.59)/y + t^8.661/(g1^21*y) + (2*g1^5*t^8.795)/y - (t^4.364*y)/g1^4 - g1^3*t^6.477*y - (t^6.682*y)/g1^2 + g1^14*t^7.226*y + g1^9*t^7.431*y - (t^7.502*y)/g1^22 + g1^4*t^7.636*y + (t^7.841*y)/g1 + (t^8.046*y)/g1^6 + g1^20*t^8.18*y + (2*t^8.251*y)/g1^11 + 2*g1^15*t^8.385*y + (t^8.456*y)/g1^16 + 2*g1^10*t^8.59*y + (t^8.661*y)/g1^21 + 2*g1^5*t^8.795*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 |
---|---|---|---|---|---|---|---|---|---|
48217 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ | 0.6814 | 0.8523 | 0.7995 | [M:[1.1632, 1.0209, 0.8368, 0.7755, 0.7141], q:[0.3877, 0.4491], qb:[0.5914, 0.7755], phi:[0.4491]] | t^2.142 + t^2.326 + t^2.51 + t^2.694 + t^3.063 + t^3.121 + t^3.49 + t^3.674 + t^4.042 + t^4.101 + 2*t^4.285 + 2*t^4.469 + 2*t^4.653 + 2*t^4.837 + t^4.896 + 2*t^5.021 + 2*t^5.205 + t^5.264 + t^5.389 + t^5.448 + 2*t^5.632 + t^5.757 + 2*t^5.816 - t^6. - t^4.347/y - t^4.347*y | detail |