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 |
---|---|---|---|---|---|---|---|---|---|
58162 | SU3adj1nf2 | ${}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }q_{2}\tilde{q}_{2}X_{2}$ | 0.8959 | 1.0047 | 0.8917 | [X:[1.4517, 1.3707], M:[1.1776], q:[0.4299, 0.2368], qb:[1.296, 0.3925], phi:[0.2741]] | [X:[[-2], [5]], M:[[-3]], q:[[4], [-4]], qb:[[-5], [-1]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{2}$, ${ }X_{1}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{5}q_{2}\tilde{q}_{2}$ | 0 | t^2.47 + t^2.71 + 3*t^3.53 + t^4.11 + t^4.36 + 2*t^4.6 + 2*t^5.18 + t^5.42 + 3*t^6.24 + 6*t^7.07 + 2*t^7.31 + t^7.64 + 2*t^7.89 + 6*t^8.13 + t^8.22 - t^8.47 + t^8.71 + 4*t^8.95 + t^8.47/y^2 - t^3.82/y - t^4.64/y - t^6.29/y - (2*t^7.36)/y - t^7.93/y - t^8.42/y - t^8.76/y - t^3.82*y - t^4.64*y - t^6.29*y - 2*t^7.36*y - t^7.93*y - t^8.42*y - t^8.76*y + t^8.47*y^2 | g1^3*t^2.47 + t^2.71/g1^4 + (3*t^3.53)/g1^3 + g1^5*t^4.11 + t^4.36/g1^2 + (2*t^4.6)/g1^9 + (2*t^5.18)/g1 + t^5.42/g1^8 + (3*t^6.24)/g1^7 + (6*t^7.07)/g1^6 + (2*t^7.31)/g1^13 + g1^2*t^7.64 + (2*t^7.89)/g1^5 + (6*t^8.13)/g1^12 + g1^10*t^8.22 - g1^3*t^8.47 + t^8.71/g1^4 + (4*t^8.95)/g1^11 + (g1^3*t^8.47)/y^2 - (g1*t^3.82)/y - (g1^2*t^4.64)/y - (g1^4*t^6.29)/y - (2*t^7.36)/(g1^2*y) - (g1^6*t^7.93)/y - t^8.42/(g1^8*y) - (g1^7*t^8.76)/y - g1*t^3.82*y - g1^2*t^4.64*y - g1^4*t^6.29*y - (2*t^7.36*y)/g1^2 - g1^6*t^7.93*y - (t^8.42*y)/g1^8 - g1^7*t^8.76*y + g1^3*t^8.47*y^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 |
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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 |
---|---|---|---|---|---|---|---|---|---|
57330 | SU3adj1nf2 | ${}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ | 1.1299 | 1.2638 | 0.8941 | [X:[1.5296], M:[0.68], q:[0.8886, 0.3926], qb:[0.8763, 0.4315], phi:[0.2352]] | t^2.04 + t^2.117 + t^2.472 + t^3.178 + t^3.806 + t^3.883 + t^4.08 + t^4.157 + t^4.233 + t^4.512 + 2*t^4.589 + t^4.944 + t^5.218 + 2*t^5.294 + 2*t^5.65 + t^5.727 + t^5.846 + 2*t^5.923 - t^6. - t^3.706/y - t^4.411/y - t^5.745/y - t^5.822/y - t^3.706*y - t^4.411*y - t^5.745*y - t^5.822*y | detail |