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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58166 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ | 1.4145 | 1.624 | 0.871 | [X:[1.2941], M:[0.8824], q:[0.4069, 0.5245], qb:[0.5931, 0.3578], phi:[0.3529]] | [X:[[0]], M:[[0]], q:[[-1], [-1]], qb:[[1], [1]], phi:[[0]]] | 1 | {a: 889497/628864, c: 1021281/628864, X1: 22/17, M1: 15/17, q1: 83/204, q2: 107/204, qb1: 121/204, qb2: 73/204, phi1: 6/17} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${}\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$ | 0 | t^2.29 + 2*t^2.65 + t^3. + t^3.18 + t^3.35 + t^3.71 + t^3.88 + t^4.06 + 2*t^4.41 + t^4.59 + t^4.76 + 2*t^4.94 + t^4.99 + t^5.07 + t^5.12 + 3*t^5.29 + t^5.43 + 2*t^5.47 + 2*t^5.65 + t^5.69 + 2*t^5.82 + t^6.04 + t^6.13 + 2*t^6.18 + 3*t^6.35 + t^6.4 + t^6.49 + 3*t^6.53 + 4*t^6.71 + t^6.75 + t^6.84 + 3*t^6.88 - t^7.01 + 5*t^7.06 + t^7.1 + t^7.19 + 3*t^7.24 + t^7.37 + 5*t^7.41 + t^7.54 + 5*t^7.59 + t^7.72 + 6*t^7.76 + t^7.81 + t^7.9 + 5*t^7.94 + t^7.99 + t^8.07 + 7*t^8.12 + t^8.16 + t^8.25 + t^8.29 + 2*t^8.34 + t^8.43 + 8*t^8.47 + t^8.51 + t^8.6 + 2*t^8.69 + t^8.78 + 8*t^8.82 + t^8.87 - t^4.06/y - t^5.12/y - t^6.35/y - (2*t^6.71)/y - t^7.06/y - t^7.24/y - t^7.41/y - (2*t^7.76)/y + (2*t^7.94)/y - t^8.12/y + t^8.29/y + (2*t^8.65)/y + t^8.82/y - t^4.06*y - t^5.12*y - t^6.35*y - 2*t^6.71*y - t^7.06*y - t^7.24*y - t^7.41*y - 2*t^7.76*y + 2*t^7.94*y - t^8.12*y + t^8.29*y + 2*t^8.65*y + t^8.82*y | t^2.29 + 2*t^2.65 + t^3. + t^3.18 + t^3.35 + t^3.71 + t^3.88 + t^4.06 + 2*t^4.41 + t^4.59 + t^4.76 + 2*t^4.94 + g1^3*t^4.99 + t^5.07/g1^3 + t^5.12 + 3*t^5.29 + t^5.43/g1^3 + 2*t^5.47 + 2*t^5.65 + g1^3*t^5.69 + 2*t^5.82 + g1^3*t^6.04 + t^6.13/g1^3 + 2*t^6.18 + 3*t^6.35 + g1^3*t^6.4 + t^6.49/g1^3 + 3*t^6.53 + 4*t^6.71 + g1^3*t^6.75 + t^6.84/g1^3 + 3*t^6.88 - t^7.01/g1^3 + 5*t^7.06 + g1^3*t^7.1 + t^7.19/g1^3 + 3*t^7.24 + t^7.37/g1^3 + 5*t^7.41 + t^7.54/g1^3 + 5*t^7.59 + t^7.72/g1^3 + 6*t^7.76 + g1^3*t^7.81 + t^7.9/g1^3 + 5*t^7.94 + g1^3*t^7.99 + t^8.07/g1^3 + 7*t^8.12 + g1^3*t^8.16 + t^8.25/g1^3 + t^8.29 + 2*g1^3*t^8.34 + t^8.43/g1^3 + 8*t^8.47 + g1^3*t^8.51 + t^8.6/g1^3 + 2*g1^3*t^8.69 + t^8.78/g1^3 + 8*t^8.82 + g1^3*t^8.87 - t^4.06/y - t^5.12/y - t^6.35/y - (2*t^6.71)/y - t^7.06/y - t^7.24/y - t^7.41/y - (2*t^7.76)/y + (2*t^7.94)/y - t^8.12/y + t^8.29/y + (2*t^8.65)/y + t^8.82/y - t^4.06*y - t^5.12*y - t^6.35*y - 2*t^6.71*y - t^7.06*y - t^7.24*y - t^7.41*y - 2*t^7.76*y + 2*t^7.94*y - t^8.12*y + t^8.29*y + 2*t^8.65*y + t^8.82*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 |
---|---|---|---|---|---|---|---|---|---|
57271 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ | 1.474 | 1.6823 | 0.8761 | [X:[1.3325], M:[0.6714], q:[0.4981, 0.5006], qb:[0.5019, 0.4968], phi:[0.3338]] | t^2.014 + t^2.984 + t^2.992 + t^3. + t^3.004 + t^3.008 + t^3.994 + t^3.997 + t^4.001 + t^4.009 + t^4.029 + t^4.987 + t^4.995 + t^4.999 + t^5.003 + t^5.006 + t^5.01 + t^5.014 + t^5.018 + t^5.022 + t^5.488 + t^5.492 + t^5.499 + t^5.503 + t^5.969 + t^5.977 + t^5.984 + t^5.988 + t^5.992 + t^5.996 - 2*t^6. - t^4.001/y - t^5.003/y - t^4.001*y - t^5.003*y | detail |