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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4080 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}q_{2}$ + ${ }M_{3}M_{7}$ + ${ }M_{4}X_{1}$ + ${ }M_{2}M_{8}$ | 0.6881 | 0.8524 | 0.8073 | [X:[1.3242], M:[1.0209, 1.1172, 0.9518, 0.6758, 0.7448, 0.8138, 1.0482, 0.8828], q:[0.7793, 0.4069], qb:[0.5722, 0.4759], phi:[0.4414]] | [X:[[18]], M:[[32], [-12], [22], [-18], [-8], [2], [-22], [12]], q:[[-3], [1]], qb:[[-33], [11]], phi:[[6]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{5}$, ${ }M_{6}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{7}$, ${ }q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}M_{8}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{8}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{5}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{1}M_{8}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{7}M_{8}$, ${ }M_{7}\phi_{1}^{2}$ | ${}$ | -2 | t^2.234 + t^2.441 + 2*t^2.648 + t^3.063 + t^3.144 + t^3.766 + t^3.973 + t^4.055 + t^4.18 + t^4.262 + 2*t^4.469 + t^4.676 + t^4.758 + 3*t^4.883 + 2*t^5.09 + 4*t^5.297 + t^5.379 + t^5.586 + t^5.711 + t^5.793 - 2*t^6. + t^6.125 + t^6.207 + t^6.289 + 3*t^6.414 + t^6.496 + 2*t^6.621 + 3*t^6.703 + 2*t^6.828 + 3*t^6.91 + t^6.992 + 3*t^7.117 + 2*t^7.199 + t^7.242 + 2*t^7.324 + 2*t^7.406 + 5*t^7.531 + 3*t^7.738 + t^7.902 + 6*t^7.945 + 2*t^8.027 - t^8.234 + 3*t^8.36 - t^8.441 + 2*t^8.523 + t^8.567 - 3*t^8.648 + t^8.73 + t^8.774 + t^8.812 + t^8.856 + 3*t^8.937 - t^4.324/y - t^6.559/y - t^6.766/y - t^6.973/y + t^7.262/y - t^7.387/y + (2*t^7.676)/y + (3*t^7.883)/y + (3*t^8.09)/y + (2*t^8.297)/y + t^8.379/y + t^8.504/y + t^8.586/y + (2*t^8.711)/y + t^8.793/y - t^4.324*y - t^6.559*y - t^6.766*y - t^6.973*y + t^7.262*y - t^7.387*y + 2*t^7.676*y + 3*t^7.883*y + 3*t^8.09*y + 2*t^8.297*y + t^8.379*y + t^8.504*y + t^8.586*y + 2*t^8.711*y + t^8.793*y | t^2.234/g1^8 + g1^2*t^2.441 + 2*g1^12*t^2.648 + g1^32*t^3.063 + t^3.144/g1^22 + g1^8*t^3.766 + g1^18*t^3.973 + t^4.055/g1^36 + g1^28*t^4.18 + t^4.262/g1^26 + (2*t^4.469)/g1^16 + t^4.676/g1^6 + t^4.758/g1^60 + 3*g1^4*t^4.883 + 2*g1^14*t^5.09 + 4*g1^24*t^5.297 + t^5.379/g1^30 + t^5.586/g1^20 + g1^44*t^5.711 + t^5.793/g1^10 - 2*t^6. + g1^64*t^6.125 + g1^10*t^6.207 + t^6.289/g1^44 + 3*g1^20*t^6.414 + t^6.496/g1^34 + 2*g1^30*t^6.621 + (3*t^6.703)/g1^24 + 2*g1^40*t^6.828 + (3*t^6.91)/g1^14 + t^6.992/g1^68 + (3*t^7.117)/g1^4 + (2*t^7.199)/g1^58 + g1^60*t^7.242 + 2*g1^6*t^7.324 + (2*t^7.406)/g1^48 + 5*g1^16*t^7.531 + 3*g1^26*t^7.738 + t^7.902/g1^82 + 6*g1^36*t^7.945 + (2*t^8.027)/g1^18 - t^8.234/g1^8 + 3*g1^56*t^8.36 - g1^2*t^8.441 + (2*t^8.523)/g1^52 + g1^66*t^8.567 - 3*g1^12*t^8.648 + t^8.73/g1^42 + g1^76*t^8.774 + t^8.812/g1^96 + g1^22*t^8.856 + (3*t^8.937)/g1^32 - (g1^6*t^4.324)/y - t^6.559/(g1^2*y) - (g1^8*t^6.766)/y - (g1^18*t^6.973)/y + t^7.262/(g1^26*y) - (g1^38*t^7.387)/y + (2*t^7.676)/(g1^6*y) + (3*g1^4*t^7.883)/y + (3*g1^14*t^8.09)/y + (2*g1^24*t^8.297)/y + t^8.379/(g1^30*y) + (g1^34*t^8.504)/y + t^8.586/(g1^20*y) + (2*g1^44*t^8.711)/y + t^8.793/(g1^10*y) - g1^6*t^4.324*y - (t^6.559*y)/g1^2 - g1^8*t^6.766*y - g1^18*t^6.973*y + (t^7.262*y)/g1^26 - g1^38*t^7.387*y + (2*t^7.676*y)/g1^6 + 3*g1^4*t^7.883*y + 3*g1^14*t^8.09*y + 2*g1^24*t^8.297*y + (t^8.379*y)/g1^30 + g1^34*t^8.504*y + (t^8.586*y)/g1^20 + 2*g1^44*t^8.711*y + (t^8.793*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 |
---|---|---|---|---|---|---|---|---|---|
1691 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}q_{2}$ + ${ }M_{3}M_{7}$ + ${ }M_{4}X_{1}$ | 0.6779 | 0.8353 | 0.8115 | [X:[1.3337], M:[1.0377, 1.1109, 0.9634, 0.6663, 0.7406, 0.8149, 1.0366], q:[0.7777, 0.4074], qb:[0.5549, 0.4817], phi:[0.4446]] | t^2.222 + t^2.445 + t^2.667 + t^3.11 + t^3.113 + t^3.333 + t^3.778 + t^3.998 + t^4.001 + t^4.221 + t^4.224 + 2*t^4.444 + t^4.663 + t^4.666 + 2*t^4.889 + t^5.112 + t^5.332 + 2*t^5.335 + 2*t^5.554 + t^5.777 - t^6. - t^4.334/y - t^4.334*y | detail |