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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61196 | SU3adj1nf2 | ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{2}\phi_{1}q_{1}q_{2}^{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.9366 | 1.1439 | 0.8187 | [X:[1.6347, 1.6826, 1.3174, 1.3653], M:[0.8174, 0.8653], q:[0.2435, 0.1956], qb:[0.1218, 0.4391], phi:[0.5]] | [X:[[-6], [3], [-3], [6]], M:[[-3], [6]], q:[[4], [-5]], qb:[[2], [-1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }X_{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }X_{4}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }X_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1 | 2*t^2.45 + 2*t^2.6 + t^3. + t^3.4 + 2*t^3.55 + 2*t^3.95 + 2*t^4.1 + 2*t^4.5 + 6*t^4.9 + 7*t^5.05 + 3*t^5.19 + t^5.45 + 2*t^5.6 + t^5.86 + t^6. + 3*t^6.14 + t^6.26 + 4*t^6.4 + 8*t^6.55 + 5*t^6.69 + t^6.81 + t^6.95 + 4*t^7.1 + 9*t^7.36 + 16*t^7.5 + 11*t^7.64 - t^7.76 + 4*t^7.79 + 5*t^7.9 + 6*t^8.05 + 5*t^8.19 + 2*t^8.31 + 2*t^8.71 + 4*t^8.74 + 10*t^8.86 - t^4.5/y - t^6./y - t^6.95/y - t^7.1/y + t^7.5/y + (2*t^7.9)/y + (5*t^8.05)/y + t^8.19/y - t^8.45/y - t^8.6/y + (2*t^8.86)/y - t^4.5*y - t^6.*y - t^6.95*y - t^7.1*y + t^7.5*y + 2*t^7.9*y + 5*t^8.05*y + t^8.19*y - t^8.45*y - t^8.6*y + 2*t^8.86*y | (2*t^2.45)/g1^3 + 2*g1^6*t^2.6 + t^3. + t^3.4/g1^6 + 2*g1^3*t^3.55 + (2*t^3.95)/g1^3 + 2*g1^6*t^4.1 + 2*t^4.5 + (6*t^4.9)/g1^6 + 7*g1^3*t^5.05 + 3*g1^12*t^5.19 + t^5.45/g1^3 + 2*g1^6*t^5.6 + t^5.86/g1^9 + t^6. + 3*g1^9*t^6.14 + t^6.26/g1^15 + (4*t^6.4)/g1^6 + 8*g1^3*t^6.55 + 5*g1^12*t^6.69 + t^6.81/g1^12 + t^6.95/g1^3 + 4*g1^6*t^7.1 + (9*t^7.36)/g1^9 + 16*t^7.5 + 11*g1^9*t^7.64 - t^7.76/g1^15 + 4*g1^18*t^7.79 + (5*t^7.9)/g1^6 + 6*g1^3*t^8.05 + 5*g1^12*t^8.19 + (2*t^8.31)/g1^12 + (2*t^8.71)/g1^18 + 4*g1^15*t^8.74 + (10*t^8.86)/g1^9 - t^4.5/y - t^6./y - t^6.95/(g1^3*y) - (g1^6*t^7.1)/y + t^7.5/y + (2*t^7.9)/(g1^6*y) + (5*g1^3*t^8.05)/y + (g1^12*t^8.19)/y - t^8.45/(g1^3*y) - (g1^6*t^8.6)/y + (2*t^8.86)/(g1^9*y) - t^4.5*y - t^6.*y - (t^6.95*y)/g1^3 - g1^6*t^7.1*y + t^7.5*y + (2*t^7.9*y)/g1^6 + 5*g1^3*t^8.05*y + g1^12*t^8.19*y - (t^8.45*y)/g1^3 - g1^6*t^8.6*y + (2*t^8.86*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 |
---|---|---|---|---|---|---|---|---|---|
59041 | SU3adj1nf2 | ${}\phi_{1}^{4}$ + ${ }q_{1}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{1}X_{2}$ + ${ }q_{1}\tilde{q}_{2}X_{3}$ + ${ }q_{2}\tilde{q}_{2}X_{4}$ + ${ }M_{1}\phi_{1}q_{1}^{2}q_{2}$ + ${ }M_{2}\phi_{1}q_{1}q_{2}^{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.0052 | 1.2248 | 0.8207 | [X:[1.4988, 1.4861, 1.5139, 1.5012], M:[0.7494, 0.7367], q:[0.246, 0.2587], qb:[0.2553, 0.2401], phi:[0.5]] | t^2.21 + t^2.25 + t^2.96 + 3*t^3. + t^3.04 + t^3.71 + t^3.75 + t^4.42 + 3*t^4.46 + 6*t^4.5 + 2*t^4.54 + t^5.17 + 5*t^5.21 + t^5.24 + 5*t^5.25 + 2*t^5.29 + 2*t^5.92 + t^5.95 + t^5.96 + t^5.99 - t^6. - t^4.5/y - t^6./y - t^4.5*y - t^6.*y | detail |