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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60962 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }M_{2}\phi_{1}^{2}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{3}q_{1}^{3}$ | 1.175 | 1.3971 | 0.841 | [X:[1.5903], M:[1.1807, 0.771], q:[0.257, 0.5219], qb:[0.6106, 0.1526], phi:[0.4097]] | [X:[[1]], M:[[2], [3]], q:[[1], [15]], qb:[[-8], [-2]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}^{2}$, ${ }X_{1}$, ${ }\phi_{1}^{4}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{2}\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}^{3}$ | 0 | t^2.02 + t^2.31 + t^2.46 + t^2.6 + t^3.25 + t^3.4 + t^3.54 + t^3.69 + t^3.83 + t^3.98 + t^4.05 + 2*t^4.34 + 2*t^4.48 + 2*t^4.63 + 2*t^4.77 + 2*t^4.92 + 3*t^5.06 + t^5.13 + t^5.21 + t^5.28 + t^5.35 + t^5.42 + 3*t^5.57 + 3*t^5.71 + 4*t^5.86 + t^6.07 + 3*t^6.14 + 3*t^6.29 + 3*t^6.36 + 2*t^6.43 + 2*t^6.51 + t^6.58 + 4*t^6.65 - t^6.72 + 5*t^6.79 + 6*t^6.94 + 7*t^7.08 + t^7.15 + 3*t^7.23 + t^7.3 + 5*t^7.37 + 2*t^7.44 + 4*t^7.52 + 5*t^7.59 + 4*t^7.66 + 4*t^7.73 + 2*t^7.81 + 6*t^7.88 + 3*t^8.02 + t^8.09 + 9*t^8.17 + 5*t^8.31 + 5*t^8.38 + 4*t^8.46 + 2*t^8.53 + 3*t^8.6 + 6*t^8.67 + 4*t^8.75 + 7*t^8.82 + 5*t^8.89 + 10*t^8.96 - t^4.23/y - t^5.46/y - t^6.25/y - t^6.54/y - t^6.83/y + t^7.34/y + t^8.42/y + t^8.57/y + (2*t^8.71)/y + (3*t^8.86)/y - t^4.23*y - t^5.46*y - t^6.25*y - t^6.54*y - t^6.83*y + t^7.34*y + t^8.42*y + t^8.57*y + 2*t^8.71*y + 3*t^8.86*y | g1^13*t^2.02 + g1^3*t^2.31 + t^2.46/g1^2 + t^2.6/g1^7 + g1^12*t^3.25 + g1^7*t^3.4 + g1^2*t^3.54 + t^3.69/g1^3 + t^3.83/g1^8 + t^3.98/g1^13 + g1^26*t^4.05 + 2*g1^16*t^4.34 + 2*g1^11*t^4.48 + 2*g1^6*t^4.63 + 2*g1*t^4.77 + (2*t^4.92)/g1^4 + (3*t^5.06)/g1^9 + g1^30*t^5.13 + t^5.21/g1^14 + g1^25*t^5.28 + t^5.35/g1^19 + g1^20*t^5.42 + 3*g1^15*t^5.57 + 3*g1^10*t^5.71 + 4*g1^5*t^5.86 + g1^39*t^6.07 + (3*t^6.14)/g1^5 + (3*t^6.29)/g1^10 + 3*g1^29*t^6.36 + (2*t^6.43)/g1^15 + 2*g1^24*t^6.51 + t^6.58/g1^20 + 4*g1^19*t^6.65 - t^6.72/g1^25 + 5*g1^14*t^6.79 + 6*g1^9*t^6.94 + 7*g1^4*t^7.08 + g1^43*t^7.15 + (3*t^7.23)/g1 + g1^38*t^7.3 + (5*t^7.37)/g1^6 + 2*g1^33*t^7.44 + (4*t^7.52)/g1^11 + 5*g1^28*t^7.59 + (4*t^7.66)/g1^16 + 4*g1^23*t^7.73 + (2*t^7.81)/g1^21 + 6*g1^18*t^7.88 + 3*g1^13*t^8.02 + g1^52*t^8.09 + 9*g1^8*t^8.17 + 5*g1^3*t^8.31 + 5*g1^42*t^8.38 + (4*t^8.46)/g1^2 + 2*g1^37*t^8.53 + (3*t^8.6)/g1^7 + 6*g1^32*t^8.67 + (4*t^8.75)/g1^12 + 7*g1^27*t^8.82 + (5*t^8.89)/g1^17 + 10*g1^22*t^8.96 - t^4.23/(g1*y) - t^5.46/(g1^2*y) - (g1^12*t^6.25)/y - (g1^2*t^6.54)/y - t^6.83/(g1^8*y) + (g1^16*t^7.34)/y + (g1^20*t^8.42)/y + (g1^15*t^8.57)/y + (2*g1^10*t^8.71)/y + (3*g1^5*t^8.86)/y - (t^4.23*y)/g1 - (t^5.46*y)/g1^2 - g1^12*t^6.25*y - g1^2*t^6.54*y - (t^6.83*y)/g1^8 + g1^16*t^7.34*y + g1^20*t^8.42*y + g1^15*t^8.57*y + 2*g1^10*t^8.71*y + 3*g1^5*t^8.86*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 |
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58880 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }M_{2}\phi_{1}^{2}q_{1}\tilde{q}_{2}$ | 1.1789 | 1.3978 | 0.8433 | [X:[1.5935], M:[1.187, 0.7806], q:[0.2257, 0.535], qb:[0.6196, 0.1808], phi:[0.4065]] | t^2.15 + t^2.34 + t^2.44 + t^2.54 + t^3.37 + t^3.46 + t^3.56 + t^3.66 + t^3.76 + t^4.16 + t^4.18 + t^4.29 + t^4.49 + 2*t^4.59 + 2*t^4.68 + 2*t^4.78 + 2*t^4.88 + 2*t^4.97 + t^5.11 + t^5.29 + t^5.38 + t^5.4 + t^5.48 + t^5.51 + t^5.61 + t^5.69 + 2*t^5.71 + 3*t^5.81 + 4*t^5.9 - 2*t^6. - t^4.22/y - t^5.44/y - t^4.22*y - t^5.44*y | detail |