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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59214 | SU3adj1nf2 | ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 0.9256 | 1.1253 | 0.8225 | [X:[1.3047, 1.3907, 1.6093, 1.6953], M:[0.8047], q:[0.2604, 0.1744], qb:[0.4349, 0.1302], phi:[0.5]] | [X:[[-3], [6], [-6], [3]], M:[[-3]], q:[[4], [-5]], qb:[[-1], [2]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }X_{3}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }X_{4}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }M_{1}\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}\tilde{q}_{2}^{3}$ | 1 | 2*t^2.41 + t^2.67 + t^3. + 2*t^3.33 + 2*t^3.59 + 2*t^3.91 + 2*t^4.17 + 2*t^4.5 + 6*t^4.83 + 5*t^5.09 + t^5.34 + t^5.41 + t^5.67 + 3*t^5.74 + t^6. + t^6.07 + t^6.26 + 5*t^6.33 + 6*t^6.59 + 3*t^6.66 + 3*t^6.84 + 3*t^6.91 + 2*t^7.17 + 11*t^7.24 + 12*t^7.5 - t^7.57 + 4*t^7.76 + 7*t^7.83 + t^8.02 + 5*t^8.09 + 8*t^8.16 + 3*t^8.34 + 4*t^8.41 + 2*t^8.48 + 10*t^8.74 + t^8.93 - t^4.5/y - t^6./y - t^6.91/y + t^7.5/y + t^7.83/y + (3*t^8.09)/y - t^8.41/y - t^8.67/y + (4*t^8.74)/y - t^4.5*y - t^6.*y - t^6.91*y + t^7.5*y + t^7.83*y + 3*t^8.09*y - t^8.41*y - t^8.67*y + 4*t^8.74*y | (2*t^2.41)/g1^3 + g1^6*t^2.67 + t^3. + (2*t^3.33)/g1^6 + 2*g1^3*t^3.59 + (2*t^3.91)/g1^3 + 2*g1^6*t^4.17 + 2*t^4.5 + (6*t^4.83)/g1^6 + 5*g1^3*t^5.09 + g1^12*t^5.34 + t^5.41/g1^3 + g1^6*t^5.67 + (3*t^5.74)/g1^9 + t^6. + t^6.07/g1^15 + g1^9*t^6.26 + (5*t^6.33)/g1^6 + 6*g1^3*t^6.59 + (3*t^6.66)/g1^12 + 3*g1^12*t^6.84 + (3*t^6.91)/g1^3 + 2*g1^6*t^7.17 + (11*t^7.24)/g1^9 + 12*t^7.5 - t^7.57/g1^15 + 4*g1^9*t^7.76 + (7*t^7.83)/g1^6 + g1^18*t^8.02 + 5*g1^3*t^8.09 + (8*t^8.16)/g1^12 + 3*g1^12*t^8.34 + (4*t^8.41)/g1^3 + (2*t^8.48)/g1^18 + (10*t^8.74)/g1^9 + g1^15*t^8.93 - t^4.5/y - t^6./y - t^6.91/(g1^3*y) + t^7.5/y + t^7.83/(g1^6*y) + (3*g1^3*t^8.09)/y - t^8.41/(g1^3*y) - (g1^6*t^8.67)/y + (4*t^8.74)/(g1^9*y) - t^4.5*y - t^6.*y - (t^6.91*y)/g1^3 + t^7.5*y + (t^7.83*y)/g1^6 + 3*g1^3*t^8.09*y - (t^8.41*y)/g1^3 - g1^6*t^8.67*y + (4*t^8.74*y)/g1^9 |
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 |
---|---|---|---|---|---|---|---|---|---|
57723 | SU3adj1nf2 | ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 0.9859 | 1.1893 | 0.829 | [X:[1.5, 1.5093, 1.4907, 1.5], M:[0.7454], q:[0.2546, 0.2454], qb:[0.2454, 0.2546], phi:[0.5]] | t^2.24 + t^2.97 + 3*t^3. + t^3.03 + 2*t^3.74 + t^3.76 + 3*t^4.47 + 5*t^4.5 + 2*t^4.53 + t^5.21 + 5*t^5.24 + 3*t^5.26 + t^5.94 + 2*t^5.97 + t^6. - t^4.5/y - t^6./y - t^4.5*y - t^6.*y | detail |