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 |
---|---|---|---|---|---|---|---|---|---|
182 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$ + ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}M_{2}$ | 0.5241 | 0.5971 | 0.8778 | [X:[1.3807], M:[0.9289, 1.0711], q:[0.5355, 1.1548], qb:[0.5355, 0.5355], phi:[0.3096]] | [X:[[4]], M:[[-6], [6]], q:[[3], [-1]], qb:[[3], [3]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }X_{1}$, ${ }q_{1}q_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$ | ${}$ | -7 | 3*t^3.213 + 4*t^4.142 + t^5.071 - 7*t^6. + 6*t^6.426 - 6*t^6.929 + 10*t^7.355 + t^7.858 + 6*t^8.284 + 4*t^8.787 - t^3.929/y - t^3.929*y | 3*g1^6*t^3.213 + 4*g1^4*t^4.142 + g1^2*t^5.071 - 7*t^6. + 6*g1^12*t^6.426 - (6*t^6.929)/g1^2 + 10*g1^10*t^7.355 + t^7.858/g1^4 + 6*g1^8*t^8.284 + (4*t^8.787)/g1^6 - t^3.929/(g1^2*y) - (t^3.929*y)/g1^2 |
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 |
---|---|---|---|---|---|---|---|---|---|
55795 | SU2adj1nf3 | ${}\phi_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{3}^{2}$ + ${ }q_{2}q_{3}$ + ${ }q_{3}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ | 0.5241 | 0.5971 | 0.8778 | [X:[1.3807], q:[0.5355, 1.1548, 0.8452], qb:[1.1548, 0.5355, 0.5355], phi:[0.3096]] | 3*t^3.213 + 4*t^4.142 + t^5.071 - 7*t^6. - t^3.929/y - t^3.929*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
117 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$ + ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 0.5336 | 0.6056 | 0.881 | [X:[1.4237], M:[0.8645], q:[0.5678, 1.1441], qb:[0.5678, 0.5678], phi:[0.2882]] | t^2.593 + 2*t^3.407 + 4*t^4.271 + t^5.136 + t^5.187 - 5*t^6. - t^3.864/y - t^3.864*y | detail |