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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61029 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{3}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{3}X_{1}$ | 1.4237 | 1.6631 | 0.856 | [X:[1.2678], M:[0.9289, 0.9017, 0.7322], q:[0.4788, 0.4077], qb:[0.5923, 0.3245], phi:[0.3661]] | [X:[[0, 2]], M:[[0, -8], [0, 3], [0, -2]], q:[[-1, 6], [-1, -2]], qb:[[1, 2], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$ | ${}$ | -2 | 2*t^2.2 + t^2.41 + t^2.71 + t^2.79 + t^3. + t^3.29 + t^3.51 + t^4.1 + t^4.31 + 4*t^4.39 + 3*t^4.61 + 2*t^4.82 + 2*t^4.9 + 3*t^4.98 + t^5.12 + t^5.19 + 3*t^5.2 + 3*t^5.41 + 3*t^5.49 + t^5.57 + t^5.63 + 4*t^5.71 + 2*t^5.92 - 2*t^6. + 2*t^6.08 + t^6.22 + 4*t^6.29 + 4*t^6.51 + 7*t^6.59 + 2*t^6.72 + 7*t^6.8 - t^6.88 + t^6.96 + 8*t^7.02 + 2*t^7.1 + 7*t^7.18 + 2*t^7.23 + t^7.31 + 11*t^7.39 + t^7.53 + 2*t^7.6 + 9*t^7.61 + 6*t^7.69 + 2*t^7.77 + 7*t^7.82 + 9*t^7.9 + t^8.04 + 9*t^8.12 - 4*t^8.2 + 6*t^8.28 + 4*t^8.33 + t^8.36 + 11*t^8.49 - t^8.57 + t^8.62 + t^8.63 + 2*t^8.7 + 8*t^8.71 - 2*t^8.78 + 9*t^8.79 + t^8.87 + 9*t^8.92 - t^4.1/y - t^5.2/y - (2*t^6.29)/y - t^6.51/y - t^6.8/y - t^6.88/y - t^7.1/y - t^7.39/y + t^7.61/y + (2*t^7.9)/y + t^7.98/y + t^8.12/y + (2*t^8.2)/y + t^8.41/y - t^8.49/y + t^8.71/y + t^8.79/y - t^4.1*y - t^5.2*y - 2*t^6.29*y - t^6.51*y - t^6.8*y - t^6.88*y - t^7.1*y - t^7.39*y + t^7.61*y + 2*t^7.9*y + t^7.98*y + t^8.12*y + 2*t^8.2*y + t^8.41*y - t^8.49*y + t^8.71*y + t^8.79*y | (2*t^2.2)/g2^2 + g2^6*t^2.41 + g2^3*t^2.71 + t^2.79/g2^8 + t^3. + t^3.29/g2^3 + g2^5*t^3.51 + t^4.1/g2 + g2^7*t^4.31 + (4*t^4.39)/g2^4 + 3*g2^4*t^4.61 + g1^3*g2*t^4.82 + g2^12*t^4.82 + 2*g2*t^4.9 + (2*t^4.98)/g2^10 + (g2*t^4.98)/g1^3 + g2^9*t^5.12 + (g2^9*t^5.19)/g1^3 + (3*t^5.2)/g2^2 + 3*g2^6*t^5.41 + (3*t^5.49)/g2^5 + t^5.57/g2^16 + g1^3*g2^3*t^5.63 + 4*g2^3*t^5.71 + g1^3*t^5.92 + g2^11*t^5.92 - 2*t^6. + t^6.08/g1^3 + t^6.08/g2^11 + (g1^3*t^6.22)/g2^3 + (3*t^6.29)/g2^3 + (g2^8*t^6.29)/g1^3 + 4*g2^5*t^6.51 + (7*t^6.59)/g2^6 + g1^3*g2^2*t^6.72 + g2^13*t^6.72 + 7*g2^2*t^6.8 - (g2^2*t^6.88)/g1^3 + t^6.96/(g1^3*g2^9) + (3*g1^3*t^7.02)/g2 + 5*g2^10*t^7.02 + (2*t^7.1)/g2 + (4*t^7.18)/g2^12 + (3*t^7.18)/(g1^3*g2) + g1^3*g2^7*t^7.23 + g2^18*t^7.23 - (g1^3*t^7.31)/g2^4 + 2*g2^7*t^7.31 + (7*t^7.39)/g2^4 + (4*g2^7*t^7.39)/g1^3 + g2^15*t^7.53 + (2*g2^15*t^7.6)/g1^3 + 9*g2^4*t^7.61 + (6*t^7.69)/g2^7 + (2*t^7.77)/g2^18 + 3*g1^3*g2*t^7.82 + 4*g2^12*t^7.82 + 8*g2*t^7.9 + (g2^12*t^7.9)/g1^3 + g1^3*g2^9*t^8.04 + (3*g1^3*t^8.12)/g2^2 + 6*g2^9*t^8.12 - (4*t^8.2)/g2^2 + (3*t^8.28)/g2^13 + (3*t^8.28)/(g1^3*g2^2) + 3*g1^3*g2^6*t^8.33 + g2^17*t^8.33 + t^8.36/g2^24 + (g1^3*t^8.41)/g2^5 - g2^6*t^8.41 + (7*t^8.49)/g2^5 + (4*g2^6*t^8.49)/g1^3 - t^8.57/(g1^3*g2^5) + g2^14*t^8.62 + g1^3*g2^3*t^8.63 + (2*g2^14*t^8.7)/g1^3 + 8*g2^3*t^8.71 - (2*g2^3*t^8.78)/g1^3 + (9*t^8.79)/g2^8 + t^8.87/g2^19 + 3*g1^3*t^8.92 + 6*g2^11*t^8.92 - t^4.1/(g2*y) - t^5.2/(g2^2*y) - (2*t^6.29)/(g2^3*y) - (g2^5*t^6.51)/y - (g2^2*t^6.8)/y - t^6.88/(g2^9*y) - t^7.1/(g2*y) - t^7.39/(g2^4*y) + (g2^4*t^7.61)/y + (2*g2*t^7.9)/y + t^7.98/(g2^10*y) + (g2^9*t^8.12)/y + (2*t^8.2)/(g2^2*y) + (g2^6*t^8.41)/y - t^8.49/(g2^5*y) + (g2^3*t^8.71)/y + t^8.79/(g2^8*y) - (t^4.1*y)/g2 - (t^5.2*y)/g2^2 - (2*t^6.29*y)/g2^3 - g2^5*t^6.51*y - g2^2*t^6.8*y - (t^6.88*y)/g2^9 - (t^7.1*y)/g2 - (t^7.39*y)/g2^4 + g2^4*t^7.61*y + 2*g2*t^7.9*y + (t^7.98*y)/g2^10 + g2^9*t^8.12*y + (2*t^8.2*y)/g2^2 + g2^6*t^8.41*y - (t^8.49*y)/g2^5 + g2^3*t^8.71*y + (t^8.79*y)/g2^8 |
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 |
---|---|---|---|---|---|---|---|---|---|
58465 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{3}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ | 1.404 | 1.6269 | 0.863 | [X:[1.2667], M:[0.933, 0.9001], q:[0.476, 0.409], qb:[0.591, 0.3243], phi:[0.3666]] | t^2.2 + t^2.4 + t^2.7 + t^2.8 + t^3. + t^3.3 + t^3.5 + t^3.8 + t^4.1 + t^4.3 + 2*t^4.4 + 2*t^4.6 + t^4.8 + t^4.82 + t^4.9 + t^4.98 + t^5. + t^5.1 + t^5.18 + 2*t^5.2 + 3*t^5.4 + 2*t^5.5 + t^5.6 + t^5.62 + 3*t^5.7 + t^5.9 + t^5.92 - t^6. - t^4.1/y - t^5.2/y - t^4.1*y - t^5.2*y | detail |