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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5154 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{7}$ + ${ }M_{8}\phi_{1}q_{2}^{2}$ | 0.6429 | 0.8033 | 0.8003 | [M:[0.8093, 1.2371, 0.7166, 0.8556, 0.6702, 1.1444, 1.1907, 0.7166], q:[0.7397, 0.451], qb:[0.4046, 0.8788], phi:[0.3815]] | [M:[[2], [8], [-18], [12], [-28], [-12], [-2], [-18]], q:[[-13], [11]], qb:[[1], [17]], phi:[[-4]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{5}$, ${ }M_{3}$, ${ }M_{8}$, ${ }M_{4}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{8}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{8}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{6}M_{8}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{7}$, ${ }M_{7}M_{8}$, ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{8}$, ${ }M_{8}\phi_{1}q_{2}\tilde{q}_{1}$ | ${}$ | -2 | t^2.011 + 2*t^2.15 + t^2.567 + t^3.433 + 2*t^3.572 + 2*t^3.711 + t^4.021 + 2*t^4.16 + 3*t^4.299 + t^4.578 + 2*t^4.717 + t^4.856 + t^5.134 + t^5.444 + 4*t^5.583 + 5*t^5.722 + 2*t^5.861 - 2*t^6. + t^6.032 + 2*t^6.171 + t^6.278 + 3*t^6.31 + 4*t^6.449 + t^6.588 + 2*t^6.727 + 4*t^6.866 + 2*t^7.005 + 3*t^7.144 + 2*t^7.283 + t^7.454 - 2*t^7.562 + 4*t^7.594 + 8*t^7.733 + 6*t^7.872 + t^8.043 - 4*t^8.15 + 2*t^8.182 + t^8.289 + 3*t^8.321 + 4*t^8.46 - 2*t^8.567 + 6*t^8.599 - 2*t^8.706 + 2*t^8.738 + 4*t^8.877 - t^4.144/y - t^6.155/y - (2*t^6.294)/y + (2*t^7.16)/y + t^7.299/y + t^7.578/y + (2*t^7.717)/y + (2*t^7.995)/y + t^8.134/y - t^8.166/y - (2*t^8.305)/y - (2*t^8.444)/y + (4*t^8.583)/y + (6*t^8.722)/y + (4*t^8.861)/y - t^4.144*y - t^6.155*y - 2*t^6.294*y + 2*t^7.16*y + t^7.299*y + t^7.578*y + 2*t^7.717*y + 2*t^7.995*y + t^8.134*y - t^8.166*y - 2*t^8.305*y - 2*t^8.444*y + 4*t^8.583*y + 6*t^8.722*y + 4*t^8.861*y | t^2.011/g1^28 + (2*t^2.15)/g1^18 + g1^12*t^2.567 + t^3.433/g1^12 + (2*t^3.572)/g1^2 + 2*g1^8*t^3.711 + t^4.021/g1^56 + (2*t^4.16)/g1^46 + (3*t^4.299)/g1^36 + t^4.578/g1^16 + (2*t^4.717)/g1^6 + g1^4*t^4.856 + g1^24*t^5.134 + t^5.444/g1^40 + (4*t^5.583)/g1^30 + (5*t^5.722)/g1^20 + (2*t^5.861)/g1^10 - 2*t^6. + t^6.032/g1^84 + (2*t^6.171)/g1^74 + g1^20*t^6.278 + (3*t^6.31)/g1^64 + (4*t^6.449)/g1^54 + t^6.588/g1^44 + (2*t^6.727)/g1^34 + (4*t^6.866)/g1^24 + (2*t^7.005)/g1^14 + (3*t^7.144)/g1^4 + 2*g1^6*t^7.283 + t^7.454/g1^68 - 2*g1^26*t^7.562 + (4*t^7.594)/g1^58 + (8*t^7.733)/g1^48 + (6*t^7.872)/g1^38 + t^8.043/g1^112 - (4*t^8.15)/g1^18 + (2*t^8.182)/g1^102 + t^8.289/g1^8 + (3*t^8.321)/g1^92 + (4*t^8.46)/g1^82 - 2*g1^12*t^8.567 + (6*t^8.599)/g1^72 - 2*g1^22*t^8.706 + (2*t^8.738)/g1^62 + (4*t^8.877)/g1^52 - t^4.144/(g1^4*y) - t^6.155/(g1^32*y) - (2*t^6.294)/(g1^22*y) + (2*t^7.16)/(g1^46*y) + t^7.299/(g1^36*y) + t^7.578/(g1^16*y) + (2*t^7.717)/(g1^6*y) + (2*g1^14*t^7.995)/y + (g1^24*t^8.134)/y - t^8.166/(g1^60*y) - (2*t^8.305)/(g1^50*y) - (2*t^8.444)/(g1^40*y) + (4*t^8.583)/(g1^30*y) + (6*t^8.722)/(g1^20*y) + (4*t^8.861)/(g1^10*y) - (t^4.144*y)/g1^4 - (t^6.155*y)/g1^32 - (2*t^6.294*y)/g1^22 + (2*t^7.16*y)/g1^46 + (t^7.299*y)/g1^36 + (t^7.578*y)/g1^16 + (2*t^7.717*y)/g1^6 + 2*g1^14*t^7.995*y + g1^24*t^8.134*y - (t^8.166*y)/g1^60 - (2*t^8.305*y)/g1^50 - (2*t^8.444*y)/g1^40 + (4*t^8.583*y)/g1^30 + (6*t^8.722*y)/g1^20 + (4*t^8.861*y)/g1^10 |
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 |
---|---|---|---|---|---|---|---|---|---|
3473 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{7}$ | 0.6228 | 0.765 | 0.8141 | [M:[0.8084, 1.2337, 0.7242, 0.8505, 0.6821, 1.1495, 1.1916], q:[0.7453, 0.4463], qb:[0.4042, 0.8716], phi:[0.3832]] | t^2.046 + t^2.173 + t^2.552 + t^3.448 + 2*t^3.575 + 2*t^3.701 + t^3.827 + t^4.093 + t^4.219 + t^4.345 + t^4.598 + t^4.724 + t^4.851 + t^5.103 + t^5.495 + 3*t^5.621 + 3*t^5.747 + t^5.874 - t^6. - t^4.149/y - t^4.149*y | detail |