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 |
---|---|---|---|---|---|---|---|---|---|
57838 | SU3adj1nf2 | ${}\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | 1.0611 | 1.158 | 0.9163 | [X:[1.5265], M:[1.2898], q:[1.0966, 0.3864], qb:[0.4299, 0.6667], phi:[0.2367]] | [X:[[2]], M:[[3]], q:[[1], [4]], qb:[[1], [0]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.45 + 2*t^3.16 + 2*t^3.87 + 2*t^4.58 + t^4.9 + t^5.29 + 3*t^5.61 - 2*t^6. + 6*t^6.32 - 3*t^6.71 + 6*t^7.03 + t^7.35 - 2*t^7.42 + 6*t^7.74 + 3*t^8.06 - t^8.13 + 8*t^8.77 + t^8.13/y^2 - t^3.71/y - t^4.42/y - t^6.16/y - (2*t^6.87)/y - (2*t^7.58)/y - (2*t^8.29)/y + t^8.61/y - t^3.71*y - t^4.42*y - t^6.16*y - 2*t^6.87*y - 2*t^7.58*y - 2*t^8.29*y + t^8.61*y + t^8.13*y^2 | g1^5*t^2.45 + 2*g1^4*t^3.16 + 2*g1^3*t^3.87 + 2*g1^2*t^4.58 + g1^10*t^4.9 + g1*t^5.29 + 3*g1^9*t^5.61 - 2*t^6. + 6*g1^8*t^6.32 - (3*t^6.71)/g1 + 6*g1^7*t^7.03 + g1^15*t^7.35 - (2*t^7.42)/g1^2 + 6*g1^6*t^7.74 + 3*g1^14*t^8.06 - t^8.13/g1^3 + 8*g1^13*t^8.77 + t^8.13/(g1^3*y^2) - t^3.71/(g1*y) - t^4.42/(g1^2*y) - (g1^4*t^6.16)/y - (2*g1^3*t^6.87)/y - (2*g1^2*t^7.58)/y - (2*g1*t^8.29)/y + (g1^9*t^8.61)/y - (t^3.71*y)/g1 - (t^4.42*y)/g1^2 - g1^4*t^6.16*y - 2*g1^3*t^6.87*y - 2*g1^2*t^7.58*y - 2*g1*t^8.29*y + g1^9*t^8.61*y + (t^8.13*y^2)/g1^3 |
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 |
---|---|---|---|---|---|---|---|---|---|
57275 | SU3adj1nf2 | ${}\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1.3035 | 1.4498 | 0.8991 | [X:[1.4213], M:[1.1319], q:[0.6582, 0.3688], qb:[0.7631, 0.4738], phi:[0.2894]] | t^2.528 + 4*t^3.396 + 5*t^4.264 + 2*t^5.055 + t^5.132 + 7*t^5.924 - 4*t^6. - t^3.868/y - t^4.736/y - t^3.868*y - t^4.736*y | detail |