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 |
---|---|---|---|---|---|---|---|---|---|
45467 | SO5adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1q_1q_2$ + $ M_3\phi_1^2q_1$ + $ M_4\phi_1^2q_2$ + $ M_5q_2^2$ + $ M_6q_1^2$ | 1.8346 | 1.9777 | 0.9276 | [X:[], M:[1.0262, 0.6842, 0.829, 0.829, 1.0262, 1.0262], q:[0.4869, 0.4869], qb:[], phi:[0.3421]] | [X:[], M:[[-3, -3], [-2, -2], [-1, 2], [2, -1], [0, -6], [-6, 0]], q:[[3, 0], [0, 3]], qb:[], phi:[[-1, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
$M_2$, $ \phi_1^2$, $ M_4$, $ M_3$, $ M_6$, $ M_5$, $ M_1$, $ M_2^2$, $ M_2\phi_1^2$, $ \phi_1^4$, $ M_2M_3$, $ M_3\phi_1^2$, $ M_2M_4$, $ M_4\phi_1^2$, $ M_4^2$, $ \phi_1^2q_1^2$, $ M_3M_4$, $ \phi_1^2q_1q_2$, $ M_3^2$, $ \phi_1^2q_2^2$, $ M_2M_5$, $ M_5\phi_1^2$, $ M_1M_2$, $ M_1\phi_1^2$, $ M_2M_6$, $ M_6\phi_1^2$, $ M_4M_5$, $ M_1M_4$, $ M_3M_5$, $ M_1M_3$, $ M_4M_6$, $ M_3M_6$ | $\phi_1^3q_1q_2$ | -3 | 2*t^2.05 + 2*t^2.49 + 3*t^3.08 + 4*t^4.1 + 4*t^4.54 + 6*t^4.97 + 6*t^5.13 + 6*t^5.57 - 3*t^6. + 12*t^6.16 + 6*t^6.59 + 9*t^7.03 + 12*t^7.18 + 10*t^7.46 + 12*t^7.62 - t^7.9 + 9*t^8.05 + 21*t^8.21 - 8*t^8.49 + 20*t^8.64 - 3*t^8.92 - t^4.03/y - (2*t^5.49)/y - (3*t^6.08)/y - (2*t^6.51)/y - (2*t^7.1)/y - (2*t^7.97)/y - (4*t^8.57)/y - t^4.03*y - 2*t^5.49*y - 3*t^6.08*y - 2*t^6.51*y - 2*t^7.1*y - 2*t^7.97*y - 4*t^8.57*y | (2*t^2.05)/(g1^2*g2^2) + (g1^2*t^2.49)/g2 + (g2^2*t^2.49)/g1 + t^3.08/g1^6 + t^3.08/g2^6 + t^3.08/(g1^3*g2^3) + (4*t^4.1)/(g1^4*g2^4) + (2*t^4.54)/g1^3 + (2*t^4.54)/g2^3 + (2*g1^4*t^4.97)/g2^2 + 2*g1*g2*t^4.97 + (2*g2^4*t^4.97)/g1^2 + (2*t^5.13)/(g1^2*g2^8) + (2*t^5.13)/(g1^5*g2^5) + (2*t^5.13)/(g1^8*g2^2) + (g1^2*t^5.57)/g2^7 + (2*t^5.57)/(g1*g2^4) + (2*t^5.57)/(g1^4*g2) + (g2^2*t^5.57)/g1^7 - t^6. - (g1^3*t^6.)/g2^3 - (g2^3*t^6.)/g1^3 + t^6.16/g1^12 + t^6.16/g2^12 + t^6.16/(g1^3*g2^9) + (8*t^6.16)/(g1^6*g2^6) + t^6.16/(g1^9*g2^3) + (3*t^6.59)/(g1^2*g2^5) + (3*t^6.59)/(g1^5*g2^2) + (3*g1^2*t^7.03)/g2^4 + (3*t^7.03)/(g1*g2) + (3*g2^2*t^7.03)/g1^4 + (4*t^7.18)/(g1^4*g2^10) + (4*t^7.18)/(g1^7*g2^7) + (4*t^7.18)/(g1^10*g2^4) + 3*g1^3*t^7.46 + (2*g1^6*t^7.46)/g2^3 + 3*g2^3*t^7.46 + (2*g2^6*t^7.46)/g1^3 + (2*t^7.62)/g1^9 + (2*t^7.62)/g2^9 + (4*t^7.62)/(g1^3*g2^6) + (4*t^7.62)/(g1^6*g2^3) - g1^4*g2^4*t^7.9 + (2*g1^4*t^8.05)/g2^8 + (g1*t^8.05)/g2^5 + (3*t^8.05)/(g1^2*g2^2) + (g2*t^8.05)/g1^5 + (2*g2^4*t^8.05)/g1^8 + (2*t^8.21)/(g1^2*g2^14) + (2*t^8.21)/(g1^5*g2^11) + (13*t^8.21)/(g1^8*g2^8) + (2*t^8.21)/(g1^11*g2^5) + (2*t^8.21)/(g1^14*g2^2) - (g1^5*t^8.49)/g2^4 - (3*g1^2*t^8.49)/g2 - (3*g2^2*t^8.49)/g1 - (g2^5*t^8.49)/g1^4 + (g1^2*t^8.64)/g2^13 + (2*t^8.64)/(g1*g2^10) + (7*t^8.64)/(g1^4*g2^7) + (7*t^8.64)/(g1^7*g2^4) + (2*t^8.64)/(g1^10*g2) + (g2^2*t^8.64)/g1^13 - g1^6*t^8.92 - g1^3*g2^3*t^8.92 - g2^6*t^8.92 - t^4.03/(g1*g2*y) - (g1^2*t^5.49)/(g2*y) - (g2^2*t^5.49)/(g1*y) - (3*t^6.08)/(g1^3*g2^3*y) - (g1*t^6.51)/(g2^2*y) - (g2*t^6.51)/(g1^2*y) - t^7.1/(g1*g2^7*y) - t^7.1/(g1^7*g2*y) - (g1^4*t^7.97)/(g2^2*y) - (g2^4*t^7.97)/(g1^2*y) + (2*t^8.13)/(g1^2*g2^8*y) - (4*t^8.13)/(g1^5*g2^5*y) + (2*t^8.13)/(g1^8*g2^2*y) - (2*t^8.57)/(g1*g2^4*y) - (2*t^8.57)/(g1^4*g2*y) - (t^4.03*y)/(g1*g2) - (g1^2*t^5.49*y)/g2 - (g2^2*t^5.49*y)/g1 - (3*t^6.08*y)/(g1^3*g2^3) - (g1*t^6.51*y)/g2^2 - (g2*t^6.51*y)/g1^2 - (t^7.1*y)/(g1*g2^7) - (t^7.1*y)/(g1^7*g2) - (g1^4*t^7.97*y)/g2^2 - (g2^4*t^7.97*y)/g1^2 + (2*t^8.13*y)/(g1^2*g2^8) - (4*t^8.13*y)/(g1^5*g2^5) + (2*t^8.13*y)/(g1^8*g2^2) - (2*t^8.57*y)/(g1*g2^4) - (2*t^8.57*y)/(g1^4*g2) |
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 |
---|---|---|---|---|---|---|---|---|
45556 | $M_1q_1q_2$ + $ M_2\phi_1q_1q_2$ + $ M_3\phi_1^2q_1$ + $ M_4\phi_1^2q_2$ + $ M_5q_2^2$ + $ M_6q_1^2$ + $ M_4M_5$ | 1.826 | 1.9661 | 0.9288 | [X:[], M:[1.0555, 0.7037, 0.7839, 0.8642, 1.1358, 0.9752], q:[0.5124, 0.4321], qb:[], phi:[0.3518]] | 2*t^2.11 + t^2.35 + t^2.59 + t^2.93 + t^3.17 + t^3.41 + 4*t^4.22 + 2*t^4.46 + 4*t^4.7 + 2*t^4.94 + 2*t^5.04 + 2*t^5.19 + 3*t^5.28 + 4*t^5.52 + t^5.76 + t^5.85 - t^4.06/y - t^5.35/y - t^5.59/y - t^4.06*y - t^5.35*y - t^5.59*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 |
---|---|---|---|---|---|---|---|---|---|
45262 | SO5adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1q_1q_2$ + $ M_3\phi_1^2q_1$ + $ M_4\phi_1^2q_2$ + $ M_5q_2^2$ | 1.8401 | 1.9862 | 0.9264 | [X:[], M:[1.0515, 0.701, 0.8445, 0.805, 1.0119], q:[0.4545, 0.494], qb:[], phi:[0.3505]] | 2*t^2.1 + t^2.41 + t^2.53 + t^2.73 + t^3.04 + t^3.15 + 4*t^4.21 + 2*t^4.52 + 2*t^4.64 + 4*t^4.83 + 2*t^4.95 + 2*t^5.07 + 3*t^5.14 + 3*t^5.26 + 2*t^5.45 + 2*t^5.57 + t^5.69 + t^5.76 - t^6. - t^4.05/y - t^5.41/y - t^5.53/y - t^4.05*y - t^5.41*y - t^5.53*y | detail |