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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58400 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ + ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ | 1.1912 | 1.4278 | 0.8343 | [X:[1.5072], M:[0.7072], q:[0.3904, 0.6048], qb:[0.5024, 0.1024], phi:[0.4]] | [X:[[3]], M:[[3]], q:[[-4], [2]], qb:[[1], [1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }X_{1}$, ${ }\phi_{1}^{4}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}^{3}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ | 3 | 2*t^2.12 + t^2.4 + 2*t^2.68 + 3*t^3.32 + t^3.6 + t^3.88 + 3*t^4.24 + 8*t^4.52 + 4*t^4.8 + 3*t^5.08 + 3*t^5.36 + 6*t^5.44 + 8*t^5.72 + 3*t^6. + 2*t^6.28 + 4*t^6.36 + 2*t^6.56 + 18*t^6.64 + 13*t^6.92 + t^7.11 + 12*t^7.2 + 5*t^7.48 + 9*t^7.56 + 6*t^7.76 + 27*t^7.84 + 3*t^8.04 + 9*t^8.12 + 9*t^8.4 + 5*t^8.49 - t^8.68 + 28*t^8.76 + 3*t^8.96 - t^4.2/y - t^5.4/y - (2*t^6.32)/y - t^6.6/y - t^6.88/y + t^7.24/y - t^7.52/y + (3*t^7.8)/y + t^8.08/y + t^8.36/y + (3*t^8.44)/y - t^4.2*y - t^5.4*y - 2*t^6.32*y - t^6.6*y - t^6.88*y + t^7.24*y - t^7.52*y + 3*t^7.8*y + t^8.08*y + t^8.36*y + 3*t^8.44*y | 2*g1^3*t^2.12 + t^2.4 + (2*t^2.68)/g1^3 + 3*g1^3*t^3.32 + t^3.6 + t^3.88/g1^3 + 3*g1^6*t^4.24 + 8*g1^3*t^4.52 + 4*t^4.8 + (3*t^5.08)/g1^3 + (3*t^5.36)/g1^6 + 6*g1^6*t^5.44 + 8*g1^3*t^5.72 + 3*t^6. + (2*t^6.28)/g1^3 + 4*g1^9*t^6.36 + (2*t^6.56)/g1^6 + 18*g1^6*t^6.64 + 13*g1^3*t^6.92 + t^7.11/g1^12 + 12*t^7.2 + (5*t^7.48)/g1^3 + 9*g1^9*t^7.56 + (6*t^7.76)/g1^6 + 27*g1^6*t^7.84 + (3*t^8.04)/g1^9 + 9*g1^3*t^8.12 + 9*t^8.4 + 5*g1^12*t^8.49 - t^8.68/g1^3 + 28*g1^9*t^8.76 + (3*t^8.96)/g1^6 - t^4.2/y - t^5.4/y - (2*g1^3*t^6.32)/y - t^6.6/y - t^6.88/(g1^3*y) + (g1^6*t^7.24)/y - (g1^3*t^7.52)/y + (3*t^7.8)/y + t^8.08/(g1^3*y) + t^8.36/(g1^6*y) + (3*g1^6*t^8.44)/y - t^4.2*y - t^5.4*y - 2*g1^3*t^6.32*y - t^6.6*y - (t^6.88*y)/g1^3 + g1^6*t^7.24*y - g1^3*t^7.52*y + 3*t^7.8*y + (t^8.08*y)/g1^3 + (t^8.36*y)/g1^6 + 3*g1^6*t^8.44*y |
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 |
---|---|---|---|---|---|---|---|---|---|
57344 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ | 1.3363 | 1.595 | 0.8378 | [M:[0.8611], q:[0.4375, 0.5812], qb:[0.3014, 0.2798], phi:[0.4]] | t^2.152 + t^2.217 + t^2.4 + 2*t^2.583 + t^2.648 + t^3.352 + t^3.6 + 2*t^3.783 + 2*t^3.848 + t^4.304 + t^4.369 + t^4.434 + 2*t^4.552 + 2*t^4.617 + 2*t^4.735 + 4*t^4.8 + t^4.865 + 4*t^4.983 + 3*t^5.048 + 3*t^5.166 + 2*t^5.231 + t^5.296 + t^5.504 + t^5.569 + 2*t^5.752 + t^5.817 + 3*t^5.935 + 2*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail |