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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61148 | SU3adj1nf2 | ${}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ | 1.1572 | 1.3116 | 0.8823 | [X:[1.5426], M:[0.6732, 0.6861, 0.9148], q:[0.8888, 0.4185], qb:[0.8825, 0.438], phi:[0.2287]] | [X:[[0, 2]], M:[[1, -2], [0, -3], [0, -4]], q:[[-1, 1], [0, 4]], qb:[[1, 0], [0, 1]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }M_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{6}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{3}$, ${ }M_{3}\phi_{1}^{3}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}$ | -2 | t^2.02 + 2*t^2.06 + t^2.57 + t^2.74 + t^3.9 + t^4.04 + 2*t^4.08 + 3*t^4.12 + t^4.59 + 3*t^4.63 + t^4.76 + 2*t^4.8 + t^5.14 + 2*t^5.31 + t^5.49 + t^5.83 + t^5.86 + t^5.92 + 2*t^5.96 - 2*t^6. - t^6.04 + t^6.06 + 2*t^6.1 + 3*t^6.14 + 4*t^6.17 + t^6.47 + t^6.61 + 4*t^6.65 + 4*t^6.69 + t^6.78 + 2*t^6.82 + 3*t^6.86 + t^7.16 + 3*t^7.2 + t^7.33 + 4*t^7.37 - t^7.41 + t^7.51 + 2*t^7.55 + t^7.71 + t^7.81 + t^7.84 + 3*t^7.88 + t^7.92 + t^7.94 + 2*t^7.98 - 2*t^8.06 + t^8.08 - 2*t^8.1 + 2*t^8.12 + 3*t^8.16 + 4*t^8.19 + 6*t^8.23 + t^8.39 + t^8.43 + t^8.49 + 3*t^8.53 - 3*t^8.57 - t^8.61 + t^8.63 + 4*t^8.67 + 3*t^8.71 - t^8.74 - t^8.78 + t^8.8 + 2*t^8.84 + 3*t^8.88 + 4*t^8.92 + t^8.06/y^2 - t^8.71/y^2 - (2*t^8.74)/y^2 - t^3.69/y - t^4.37/y - t^5.71/y - (2*t^5.74)/y - t^6.26/y - t^6.39/y - (3*t^6.43)/y + (2*t^7.08)/y + (3*t^7.63)/y - t^7.73/y - t^7.76/y - t^7.8/y - t^8.28/y + t^8.35/y - t^8.41/y - (3*t^8.45)/y - (5*t^8.49)/y - t^8.83/y + t^8.92/y + (2*t^8.96)/y - t^3.69*y - t^4.37*y - t^5.71*y - 2*t^5.74*y - t^6.26*y - t^6.39*y - 3*t^6.43*y + 2*t^7.08*y + 3*t^7.63*y - t^7.73*y - t^7.76*y - t^7.8*y - t^8.28*y + t^8.35*y - t^8.41*y - 3*t^8.45*y - 5*t^8.49*y - t^8.83*y + t^8.92*y + 2*t^8.96*y + t^8.06*y^2 - t^8.71*y^2 - 2*t^8.74*y^2 | (g1*t^2.02)/g2^2 + (2*t^2.06)/g2^3 + g2^5*t^2.57 + t^2.74/g2^4 + g1*g2^4*t^3.9 + (g1^2*t^4.04)/g2^4 + (2*g1*t^4.08)/g2^5 + (3*t^4.12)/g2^6 + g1*g2^3*t^4.59 + 3*g2^2*t^4.63 + (g1*t^4.76)/g2^6 + (2*t^4.8)/g2^7 + g2^10*t^5.14 + 2*g2*t^5.31 + t^5.49/g2^8 + g2^9*t^5.83 + (g2^8*t^5.86)/g1 + g1^2*g2^2*t^5.92 + 2*g1*g2*t^5.96 - 2*t^6. - t^6.04/(g1*g2) + (g1^3*t^6.06)/g2^6 + (2*g1^2*t^6.1)/g2^7 + (3*g1*t^6.14)/g2^8 + (4*t^6.17)/g2^9 + g1*g2^9*t^6.47 + g1^2*g2*t^6.61 + 4*g1*t^6.65 + (4*t^6.69)/g2 + (g1^2*t^6.78)/g2^8 + (2*g1*t^6.82)/g2^9 + (3*t^6.86)/g2^10 + g1*g2^8*t^7.16 + 3*g2^7*t^7.2 + (g1*t^7.33)/g2 + (4*t^7.37)/g2^2 - t^7.41/(g1*g2^3) + (g1*t^7.51)/g2^10 + (2*t^7.55)/g2^11 + g2^15*t^7.71 + g1^2*g2^8*t^7.81 + g1*g2^7*t^7.84 + 3*g2^6*t^7.88 + (g2^5*t^7.92)/g1 + g1^3*t^7.94 + (2*g1^2*t^7.98)/g2 - (2*t^8.06)/g2^3 + (g1^4*t^8.08)/g2^8 - (2*t^8.1)/(g1*g2^4) + (2*g1^3*t^8.12)/g2^9 + (3*g1^2*t^8.16)/g2^10 + (4*g1*t^8.19)/g2^11 + (6*t^8.23)/g2^12 + g2^14*t^8.39 + (g2^13*t^8.43)/g1 + g1^2*g2^7*t^8.49 + 3*g1*g2^6*t^8.53 - 3*g2^5*t^8.57 - (g2^4*t^8.61)/g1 + (g1^3*t^8.63)/g2 + (4*g1^2*t^8.67)/g2^2 + (3*g1*t^8.71)/g2^3 - t^8.74/g2^4 - t^8.78/(g1*g2^5) + (g1^3*t^8.8)/g2^10 + (2*g1^2*t^8.84)/g2^11 + (3*g1*t^8.88)/g2^12 + (4*t^8.92)/g2^13 + t^8.06/(g2^3*y^2) - (g1*t^8.71)/(g2^3*y^2) - (2*t^8.74)/(g2^4*y^2) - t^3.69/(g2*y) - t^4.37/(g2^2*y) - (g1*t^5.71)/(g2^3*y) - (2*t^5.74)/(g2^4*y) - (g2^4*t^6.26)/y - (g1*t^6.39)/(g2^4*y) - (3*t^6.43)/(g2^5*y) + (2*g1*t^7.08)/(g2^5*y) + (3*g2^2*t^7.63)/y - (g1^2*t^7.73)/(g2^5*y) - (g1*t^7.76)/(g2^6*y) - t^7.8/(g2^7*y) - (g1*g2^2*t^8.28)/y + t^8.35/(g1*y) - (g1^2*t^8.41)/(g2^6*y) - (3*g1*t^8.45)/(g2^7*y) - (5*t^8.49)/(g2^8*y) - (g2^9*t^8.83)/y + (g1^2*g2^2*t^8.92)/y + (2*g1*g2*t^8.96)/y - (t^3.69*y)/g2 - (t^4.37*y)/g2^2 - (g1*t^5.71*y)/g2^3 - (2*t^5.74*y)/g2^4 - g2^4*t^6.26*y - (g1*t^6.39*y)/g2^4 - (3*t^6.43*y)/g2^5 + (2*g1*t^7.08*y)/g2^5 + 3*g2^2*t^7.63*y - (g1^2*t^7.73*y)/g2^5 - (g1*t^7.76*y)/g2^6 - (t^7.8*y)/g2^7 - g1*g2^2*t^8.28*y + (t^8.35*y)/g1 - (g1^2*t^8.41*y)/g2^6 - (3*g1*t^8.45*y)/g2^7 - (5*t^8.49*y)/g2^8 - g2^9*t^8.83*y + g1^2*g2^2*t^8.92*y + 2*g1*g2*t^8.96*y + (t^8.06*y^2)/g2^3 - (g1*t^8.71*y^2)/g2^3 - (2*t^8.74*y^2)/g2^4 |
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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58079 | SU3adj1nf2 | ${}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}q_{2}\tilde{q}_{2}$ | 1.1504 | 1.3022 | 0.8834 | [X:[1.5315], M:[0.679, 0.7027], q:[0.8886, 0.3964], qb:[0.8772, 0.4324], phi:[0.2342]] | t^2.04 + 2*t^2.11 + t^2.49 + t^3.19 + t^3.82 + t^4.07 + 2*t^4.14 + 3*t^4.22 + t^4.52 + 3*t^4.59 + t^4.97 + t^5.23 + 3*t^5.3 + 2*t^5.68 + t^5.75 + t^5.86 + 2*t^5.93 - 2*t^6. - t^3.7/y - t^4.41/y - t^5.74/y - (2*t^5.81)/y - t^3.7*y - t^4.41*y - t^5.74*y - 2*t^5.81*y | detail |