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 |
---|---|---|---|---|---|---|---|---|---|
45892 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ \phi_1^2q_2\tilde{q}_2$ | 0.7546 | 0.9174 | 0.8226 | [X:[], M:[0.7904, 0.7904, 0.7904], q:[0.6048, 0.6048], qb:[0.6048, 0.6048], phi:[0.3952]] | [X:[], M:[[-4, 1, -2], [-2, 0, -2], [0, -1, -2]], q:[[2, -1, 2], [2, 0, 0]], qb:[[0, 1, 0], [0, 0, 2]], phi:[[-1, 0, -1]]] | 3 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
$M_2$, $ \phi_1^2$, $ M_3$, $ M_1$, $ q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ q_1\tilde{q}_2$, $ M_2^2$, $ M_1M_3$, $ M_2\phi_1^2$, $ \phi_1^4$, $ M_3^2$, $ M_2M_3$, $ M_3\phi_1^2$, $ M_1M_2$, $ M_1\phi_1^2$, $ M_1^2$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_1q_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_1^2$, $ \phi_1q_1\tilde{q}_2$ | $M_2q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_3q_1\tilde{q}_2$, $ \phi_1^2q_1\tilde{q}_2$, $ M_2q_2\tilde{q}_2$, $ M_3q_2\tilde{q}_2$ | -4 | 4*t^2.37 + 3*t^3.63 + 10*t^4.74 + 10*t^4.81 - 4*t^6. + 20*t^7.11 + 25*t^7.19 + 5*t^7.26 - 24*t^8.37 + 5*t^8.44 - t^4.19/y - (4*t^6.56)/y + (6*t^7.74)/y + (4*t^7.81)/y - (10*t^8.93)/y - t^4.19*y - 4*t^6.56*y + 6*t^7.74*y + 4*t^7.81*y - 10*t^8.93*y | (2*t^2.37)/(g1^2*g3^2) + t^2.37/(g2*g3^2) + (g2*t^2.37)/(g1^4*g3^2) + g1^2*g2*t^3.63 + g1^2*g3^2*t^3.63 + (g1^2*g3^4*t^3.63)/g2 + (4*t^4.74)/(g1^4*g3^4) + t^4.74/(g2^2*g3^4) + (2*t^4.74)/(g1^2*g2*g3^4) + (2*g2*t^4.74)/(g1^6*g3^4) + (g2^2*t^4.74)/(g1^8*g3^4) + (g1^3*t^4.81)/g3 + (g1*g2*t^4.81)/g3 + (g2^2*t^4.81)/(g1*g3) + 2*g1*g3*t^4.81 + (g1^3*g3*t^4.81)/g2 + (g2*g3*t^4.81)/g1 + (g3^3*t^4.81)/g1 + (g1^3*g3^3*t^4.81)/g2^2 + (g1*g3^3*t^4.81)/g2 - 2*t^6. - (g1^2*t^6.)/g2 - (g2*t^6.)/g1^2 + (6*t^7.11)/(g1^6*g3^6) + t^7.11/(g2^3*g3^6) + (2*t^7.11)/(g1^2*g2^2*g3^6) + (4*t^7.11)/(g1^4*g2*g3^6) + (4*g2*t^7.11)/(g1^8*g3^6) + (2*g2^2*t^7.11)/(g1^10*g3^6) + (g2^3*t^7.11)/(g1^12*g3^6) + (2*g1*t^7.19)/g3^3 + (g1^3*t^7.19)/(g2*g3^3) + (2*g2*t^7.19)/(g1*g3^3) + (2*g2^2*t^7.19)/(g1^3*g3^3) + (g2^3*t^7.19)/(g1^5*g3^3) + (3*t^7.19)/(g1*g3) + (g1^3*t^7.19)/(g2^2*g3) + (2*g1*t^7.19)/(g2*g3) + (2*g2*t^7.19)/(g1^3*g3) + (g2^2*t^7.19)/(g1^5*g3) + (2*g3*t^7.19)/g1^3 + (g1^3*g3*t^7.19)/g2^3 + (2*g1*g3*t^7.19)/g2^2 + (2*g3*t^7.19)/(g1*g2) + (g2*g3*t^7.19)/g1^5 + g1^4*g2^2*t^7.26 + g1^4*g2*g3^2*t^7.26 + g1^4*g3^4*t^7.26 + (g1^4*g3^6*t^7.26)/g2 + (g1^4*g3^8*t^7.26)/g2^2 - t^8.37/g1^4 - t^8.37/g2^2 - t^8.37/(g1^2*g2) - t^8.37/g3^4 - (g2*t^8.37)/(g1^2*g3^4) - (g2^2*t^8.37)/(g1^4*g3^4) - (6*t^8.37)/(g1^2*g3^2) - (g1^2*t^8.37)/(g2^2*g3^2) - (5*t^8.37)/(g2*g3^2) - (5*g2*t^8.37)/(g1^4*g3^2) - (g2^2*t^8.37)/(g1^6*g3^2) + (g1^5*g2*t^8.44)/g3 + (g1^3*g2^2*t^8.44)/g3 + (g1*g2^3*t^8.44)/g3 - g1^3*g3^3*t^8.44 + (g1^5*g3^7*t^8.44)/g2^3 + (g1^3*g3^7*t^8.44)/g2^2 + (g1*g3^7*t^8.44)/g2 - t^4.19/(g1*g3*y) - (2*t^6.56)/(g1^3*g3^3*y) - t^6.56/(g1*g2*g3^3*y) - (g2*t^6.56)/(g1^5*g3^3*y) + (2*t^7.74)/(g1^4*g3^4*y) + (2*t^7.74)/(g1^2*g2*g3^4*y) + (2*g2*t^7.74)/(g1^6*g3^4*y) + (2*g1*g3*t^7.81)/y + (g1^3*g3*t^7.81)/(g2*y) + (g2*g3*t^7.81)/(g1*y) - (4*t^8.93)/(g1^5*g3^5*y) - t^8.93/(g1*g2^2*g3^5*y) - (2*t^8.93)/(g1^3*g2*g3^5*y) - (2*g2*t^8.93)/(g1^7*g3^5*y) - (g2^2*t^8.93)/(g1^9*g3^5*y) - (t^4.19*y)/(g1*g3) - (2*t^6.56*y)/(g1^3*g3^3) - (t^6.56*y)/(g1*g2*g3^3) - (g2*t^6.56*y)/(g1^5*g3^3) + (2*t^7.74*y)/(g1^4*g3^4) + (2*t^7.74*y)/(g1^2*g2*g3^4) + (2*g2*t^7.74*y)/(g1^6*g3^4) + 2*g1*g3*t^7.81*y + (g1^3*g3*t^7.81*y)/g2 + (g2*g3*t^7.81*y)/g1 - (4*t^8.93*y)/(g1^5*g3^5) - (t^8.93*y)/(g1*g2^2*g3^5) - (2*t^8.93*y)/(g1^3*g2*g3^5) - (2*g2*t^8.93*y)/(g1^7*g3^5) - (g2^2*t^8.93*y)/(g1^9*g3^5) |
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 |
---|---|---|---|---|---|---|---|---|
46053 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ \phi_1^2q_2\tilde{q}_2$ + $ M_3^2$ | 0.7289 | 0.8891 | 0.8198 | [X:[], M:[0.7491, 0.8745, 1.0], q:[0.6255, 0.6255], qb:[0.5, 0.5], phi:[0.4373]] | t^2.25 + 2*t^2.62 + t^3. + 3*t^3.38 + 3*t^4.31 + t^4.49 + 4*t^4.69 + 2*t^4.87 + 3*t^5.06 + 4*t^5.25 + t^5.62 - t^6. - t^4.31/y - t^4.31*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
45846 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ | 0.7556 | 0.9204 | 0.821 | [X:[], M:[0.7942, 0.7604, 0.7942], q:[0.6198, 0.586], qb:[0.6198, 0.586], phi:[0.3971]] | t^2.28 + 3*t^2.38 + t^3.52 + 2*t^3.62 + t^4.56 + 3*t^4.66 + 3*t^4.71 + 6*t^4.77 + 4*t^4.81 + 3*t^4.91 + t^5.8 + t^5.9 - 2*t^6. - t^4.19/y - t^4.19*y | detail |