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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8229 | Sp2adj1nf1 | $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ M_2\phi_1^2q_1q_2$ | 1.1885 | 1.3327 | 0.8918 | [X:[1.6383], M:[0.8618, 0.7234], q:[0.4787, 0.4363], qb:[], phi:[0.1808]] | [X:[[0, 2]], M:[[2, -11], [0, -4]], q:[[-1, 6], [1, 0]], qb:[], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
$M_2$, $ \phi_1^4$, $ M_1$, $ q_1q_2$, $ \phi_1q_2^2$, $ \phi_1q_1q_2$, $ \phi_1^3q_2^2$, $ M_2^2$, $ M_2\phi_1^4$, $ \phi_1^8$, $ \phi_1^3q_1q_2$, $ \phi_1^3q_1^2$, $ M_1M_2$, $ M_1\phi_1^4$, $ M_2q_1q_2$, $ \phi_1^4q_1q_2$, $ X_1$, $ M_1^2$, $ M_1q_1q_2$, $ M_2\phi_1q_2^2$, $ \phi_1^5q_2^2$, $ M_2\phi_1q_1q_2$, $ \phi_1^5q_1q_2$, $ q_1^2q_2^2$, $ M_1\phi_1q_2^2$, $ \phi_1q_1q_2^3$ | . | -2 | 2*t^2.17 + t^2.59 + t^2.74 + t^3.16 + t^3.29 + t^4.25 + 3*t^4.34 + t^4.37 + t^4.5 + 2*t^4.76 + 3*t^4.91 + t^5.17 + 3*t^5.33 + 2*t^5.46 + t^5.49 + t^5.75 + t^5.91 - 2*t^6. + t^6.03 - t^6.13 + t^6.32 + t^6.42 + t^6.45 + 4*t^6.51 + t^6.54 + t^6.57 + t^6.67 + t^6.83 + 3*t^6.93 + t^6.99 + 5*t^7.09 + t^7.12 - t^7.21 + t^7.24 + 2*t^7.34 + t^7.41 + 5*t^7.5 + 2*t^7.53 + 2*t^7.63 + 4*t^7.66 - t^7.75 + t^7.76 + t^7.79 + 3*t^7.92 + 3*t^8.08 - 3*t^8.17 + 2*t^8.2 + t^8.23 - 2*t^8.3 + 4*t^8.49 - t^8.59 + 3*t^8.62 + t^8.65 + 5*t^8.68 - 3*t^8.71 + t^8.78 + t^8.84 + t^8.91 + t^8.17/y^2 - (2*t^8.71)/y^2 - t^3.54/y - t^4.63/y - (2*t^5.71)/y - t^6.13/y - t^6.29/y - t^6.7/y - (2*t^6.8)/y - t^6.83/y - t^7.21/y + t^7.34/y + (2*t^7.76)/y - t^7.79/y - (3*t^7.88)/y + t^7.91/y - (2*t^8.3)/y + (3*t^8.33)/y + t^8.46/y - t^8.71/y + t^8.75/y - (2*t^8.87)/y + t^8.91/y - (3*t^8.97)/y - t^3.54*y - t^4.63*y - 2*t^5.71*y - t^6.13*y - t^6.29*y - t^6.7*y - 2*t^6.8*y - t^6.83*y - t^7.21*y + t^7.34*y + 2*t^7.76*y - t^7.79*y - 3*t^7.88*y + t^7.91*y - 2*t^8.3*y + 3*t^8.33*y + t^8.46*y - t^8.71*y + t^8.75*y - 2*t^8.87*y + t^8.91*y - 3*t^8.97*y + t^8.17*y^2 - 2*t^8.71*y^2 | (2*t^2.17)/g2^4 + (g1^2*t^2.59)/g2^11 + g2^6*t^2.74 + (g1^2*t^3.16)/g2 + g2^5*t^3.29 + (g1^2*t^4.25)/g2^3 + (3*t^4.34)/g2^8 + g2^3*t^4.37 + (g2^9*t^4.5)/g1^2 + (2*g1^2*t^4.76)/g2^15 + 3*g2^2*t^4.91 + (g1^4*t^5.17)/g2^22 + (3*g1^2*t^5.33)/g2^5 + 2*g2*t^5.46 + g2^12*t^5.49 + (g1^4*t^5.75)/g2^12 + g1^2*g2^5*t^5.91 - 2*t^6. + g2^11*t^6.03 - (g2^6*t^6.13)/g1^2 + (g1^4*t^6.32)/g2^2 + (g1^2*t^6.42)/g2^7 + g1^2*g2^4*t^6.45 + (4*t^6.51)/g2^12 + t^6.54/g2 + g2^10*t^6.57 + (g2^5*t^6.67)/g1^2 + (g1^4*t^6.83)/g2^14 + (3*g1^2*t^6.93)/g2^19 + g1^2*g2^3*t^6.99 + (5*t^7.09)/g2^2 + g2^9*t^7.12 - (g2^4*t^7.21)/g1^2 + (g2^15*t^7.24)/g1^2 + (2*g1^4*t^7.34)/g2^26 + (g1^4*t^7.41)/g2^4 + (5*g1^2*t^7.5)/g2^9 + 2*g1^2*g2^2*t^7.53 + (2*t^7.63)/g2^3 + 4*g2^8*t^7.66 - (g2^3*t^7.75)/g1^2 + (g1^6*t^7.76)/g2^33 + (g2^14*t^7.79)/g1^2 + (3*g1^4*t^7.92)/g2^16 + 3*g1^2*g2*t^8.08 - (3*t^8.17)/g2^4 + 2*g2^7*t^8.2 + g2^18*t^8.23 - (2*g2^2*t^8.3)/g1^2 + (g1^6*t^8.33)/g2^23 - (g2^13*t^8.33)/g1^2 + (4*g1^4*t^8.49)/g2^6 - (g1^2*t^8.59)/g2^11 + 3*g1^2*t^8.62 + g1^2*g2^11*t^8.65 + (5*t^8.68)/g2^16 - (3*t^8.71)/g2^5 + g2^17*t^8.78 + (g2*t^8.84)/g1^2 + (g1^6*t^8.91)/g2^13 + t^8.17/(g2^4*y^2) - (2*t^8.71)/(g2^5*y^2) - t^3.54/(g2*y) - t^4.63/(g2^3*y) - (2*t^5.71)/(g2^5*y) - (g1^2*t^6.13)/(g2^12*y) - (g2^5*t^6.29)/y - (g1^2*t^6.7)/(g2^2*y) - (2*t^6.8)/(g2^7*y) - (g2^4*t^6.83)/y - (g1^2*t^7.21)/(g2^14*y) + t^7.34/(g2^8*y) + (2*g1^2*t^7.76)/(g2^15*y) - (g1^2*t^7.79)/(g2^4*y) - (3*t^7.88)/(g2^9*y) + (g2^2*t^7.91)/y - (2*g1^2*t^8.3)/(g2^16*y) + (3*g1^2*t^8.33)/(g2^5*y) + (g2*t^8.46)/y - (g1^4*t^8.71)/(g2^23*y) + (g1^4*t^8.75)/(g2^12*y) - (2*g1^2*t^8.87)/(g2^6*y) + (g1^2*g2^5*t^8.91)/y - (3*t^8.97)/(g2^11*y) - (t^3.54*y)/g2 - (t^4.63*y)/g2^3 - (2*t^5.71*y)/g2^5 - (g1^2*t^6.13*y)/g2^12 - g2^5*t^6.29*y - (g1^2*t^6.7*y)/g2^2 - (2*t^6.8*y)/g2^7 - g2^4*t^6.83*y - (g1^2*t^7.21*y)/g2^14 + (t^7.34*y)/g2^8 + (2*g1^2*t^7.76*y)/g2^15 - (g1^2*t^7.79*y)/g2^4 - (3*t^7.88*y)/g2^9 + g2^2*t^7.91*y - (2*g1^2*t^8.3*y)/g2^16 + (3*g1^2*t^8.33*y)/g2^5 + g2*t^8.46*y - (g1^4*t^8.71*y)/g2^23 + (g1^4*t^8.75*y)/g2^12 - (2*g1^2*t^8.87*y)/g2^6 + g1^2*g2^5*t^8.91*y - (3*t^8.97*y)/g2^11 + (t^8.17*y^2)/g2^4 - (2*t^8.71*y^2)/g2^5 |
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 |
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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 |
---|---|---|---|---|---|---|---|---|---|
8191 | Sp2adj1nf1 | $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ | 1.1686 | 1.2966 | 0.9013 | [X:[1.6354], M:[0.8685], q:[0.4746, 0.4317], qb:[], phi:[0.1823]] | t^2.19 + t^2.61 + t^2.72 + t^3.14 + t^3.27 + t^3.81 + t^4.23 + t^4.36 + t^4.37 + t^4.49 + t^4.79 + 2*t^4.91 + t^5.21 + 2*t^5.32 + t^5.44 + t^5.45 + t^5.74 + t^5.86 + t^5.98 - t^6. - t^3.55/y - t^4.64/y - t^5.73/y - t^3.55*y - t^4.64*y - t^5.73*y | detail |