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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5801 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_1$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_2\tilde{q}_1$ + $ M_6^2$ + $ M_3M_4$ + $ M_7\phi_1\tilde{q}_1^2$ + $ M_3M_8$ + $ M_2M_7$ + $ M_9q_1\tilde{q}_2$ | 0.7229 | 0.9121 | 0.7925 | [X:[], M:[0.6867, 1.1429, 1.0276, 0.9724, 0.7419, 1.0, 0.8571, 0.9724, 0.7143], q:[0.6704, 0.6429], qb:[0.3571, 0.6153], phi:[0.4286]] | [X:[], M:[[1], [0], [-1], [1], [-1], [0], [0], [1], [0]], q:[[-1], [0]], qb:[[0], [1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_1$, $ M_9$, $ M_5$, $ M_7$, $ M_4$, $ M_8$, $ M_6$, $ M_2$, $ M_1^2$, $ M_1M_9$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1M_5$, $ M_9^2$, $ \phi_1q_2\tilde{q}_1$, $ M_5M_9$, $ \phi_1q_1\tilde{q}_1$, $ M_5^2$, $ M_1M_7$, $ M_7M_9$, $ M_5M_7$, $ M_1M_4$, $ M_1M_8$, $ \phi_1\tilde{q}_2^2$, $ M_1M_6$, $ M_4M_9$, $ M_8M_9$, $ \phi_1q_2\tilde{q}_2$, $ M_4M_5$, $ M_7^2$, $ M_5M_8$, $ M_6M_9$, $ \phi_1q_2^2$, $ \phi_1q_1\tilde{q}_2$, $ M_5M_6$, $ \phi_1q_1q_2$, $ \phi_1q_1^2$, $ M_1M_2$, $ M_4M_7$, $ M_7M_8$, $ M_6M_7$, $ M_2M_9$, $ M_2M_5$, $ M_4^2$, $ M_4M_8$, $ M_8^2$ | . | -2 | t^2.06 + t^2.14 + t^2.23 + t^2.57 + 2*t^2.92 + t^3. + t^3.43 + t^4.12 + 2*t^4.2 + 3*t^4.29 + 2*t^4.37 + t^4.45 + t^4.63 + t^4.71 + t^4.8 + 3*t^4.98 + 3*t^5.06 + 5*t^5.14 + t^5.23 + t^5.31 + 3*t^5.49 + 2*t^5.57 + t^5.65 + 2*t^5.83 - 2*t^6. - 2*t^6.08 - t^6.17 + t^6.18 + 2*t^6.26 + 5*t^6.35 + 5*t^6.43 + 3*t^6.51 + 2*t^6.59 + t^6.68 + t^6.69 + t^6.77 + t^6.86 + t^6.94 + t^7.02 + 3*t^7.04 + 5*t^7.12 + 8*t^7.2 + 5*t^7.29 + 4*t^7.37 + t^7.45 + t^7.53 + 4*t^7.55 + 4*t^7.63 + 7*t^7.71 + 2*t^7.8 + 2*t^7.88 + 4*t^7.89 + 3*t^7.98 + 2*t^8.06 - 4*t^8.14 - 5*t^8.23 + t^8.24 - 2*t^8.31 + 2*t^8.32 - t^8.39 + 7*t^8.41 + 6*t^8.49 + 4*t^8.57 + 2*t^8.65 + 2*t^8.74 + 3*t^8.75 + 2*t^8.82 + t^8.9 - 5*t^8.92 - t^4.29/y - t^6.35/y - t^6.43/y - t^6.51/y - t^6.86/y + t^7.29/y + (2*t^7.37)/y + t^7.63/y + (2*t^7.71)/y + t^7.8/y + (2*t^7.98)/y + (4*t^8.06)/y + (4*t^8.14)/y + (2*t^8.23)/y - t^8.41/y + (2*t^8.49)/y - t^8.74/y + t^8.83/y + t^8.92/y - t^4.29*y - t^6.35*y - t^6.43*y - t^6.51*y - t^6.86*y + t^7.29*y + 2*t^7.37*y + t^7.63*y + 2*t^7.71*y + t^7.8*y + 2*t^7.98*y + 4*t^8.06*y + 4*t^8.14*y + 2*t^8.23*y - t^8.41*y + 2*t^8.49*y - t^8.74*y + t^8.83*y + t^8.92*y | g1*t^2.06 + t^2.14 + t^2.23/g1 + t^2.57 + 2*g1*t^2.92 + t^3. + t^3.43 + g1^2*t^4.12 + 2*g1*t^4.2 + 3*t^4.29 + (2*t^4.37)/g1 + t^4.45/g1^2 + g1*t^4.63 + t^4.71 + t^4.8/g1 + 3*g1^2*t^4.98 + 3*g1*t^5.06 + 5*t^5.14 + t^5.23/g1 + t^5.31/g1^2 + 3*g1*t^5.49 + 2*t^5.57 + t^5.65/g1 + 2*g1^2*t^5.83 - 2*t^6. - (2*t^6.08)/g1 - t^6.17/g1^2 + g1^3*t^6.18 + 2*g1^2*t^6.26 + 5*g1*t^6.35 + 5*t^6.43 + (3*t^6.51)/g1 + (2*t^6.59)/g1^2 + t^6.68/g1^3 + g1^2*t^6.69 + g1*t^6.77 + t^6.86 + t^6.94/g1 + t^7.02/g1^2 + 3*g1^3*t^7.04 + 5*g1^2*t^7.12 + 8*g1*t^7.2 + 5*t^7.29 + (4*t^7.37)/g1 + t^7.45/g1^2 + t^7.53/g1^3 + 4*g1^2*t^7.55 + 4*g1*t^7.63 + 7*t^7.71 + (2*t^7.8)/g1 + (2*t^7.88)/g1^2 + 4*g1^3*t^7.89 + 3*g1^2*t^7.98 + 2*g1*t^8.06 - 4*t^8.14 - (5*t^8.23)/g1 + g1^4*t^8.24 - (2*t^8.31)/g1^2 + 2*g1^3*t^8.32 - t^8.39/g1^3 + 7*g1^2*t^8.41 + 6*g1*t^8.49 + 4*t^8.57 + (2*t^8.65)/g1 + (2*t^8.74)/g1^2 + 3*g1^3*t^8.75 + (2*t^8.82)/g1^3 + t^8.9/g1^4 - 5*g1*t^8.92 - t^4.29/y - (g1*t^6.35)/y - t^6.43/y - t^6.51/(g1*y) - t^6.86/y + t^7.29/y + (2*t^7.37)/(g1*y) + (g1*t^7.63)/y + (2*t^7.71)/y + t^7.8/(g1*y) + (2*g1^2*t^7.98)/y + (4*g1*t^8.06)/y + (4*t^8.14)/y + (2*t^8.23)/(g1*y) - (g1^2*t^8.41)/y + (2*g1*t^8.49)/y - t^8.74/(g1^2*y) + (g1^2*t^8.83)/y + (g1*t^8.92)/y - t^4.29*y - g1*t^6.35*y - t^6.43*y - (t^6.51*y)/g1 - t^6.86*y + t^7.29*y + (2*t^7.37*y)/g1 + g1*t^7.63*y + 2*t^7.71*y + (t^7.8*y)/g1 + 2*g1^2*t^7.98*y + 4*g1*t^8.06*y + 4*t^8.14*y + (2*t^8.23*y)/g1 - g1^2*t^8.41*y + 2*g1*t^8.49*y - (t^8.74*y)/g1^2 + g1^2*t^8.83*y + g1*t^8.92*y |
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 |
---|---|---|---|---|---|---|---|---|---|
4355 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_1$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_2\tilde{q}_1$ + $ M_6^2$ + $ M_3M_4$ + $ M_7\phi_1\tilde{q}_1^2$ + $ M_3M_8$ + $ M_2M_7$ | 0.7026 | 0.874 | 0.8039 | [X:[], M:[0.6867, 1.1429, 1.0276, 0.9724, 0.7419, 1.0, 0.8571, 0.9724], q:[0.6704, 0.6429], qb:[0.3571, 0.6153], phi:[0.4286]] | t^2.06 + t^2.23 + t^2.57 + 2*t^2.92 + t^3. + t^3.43 + t^3.86 + t^4.12 + t^4.2 + 2*t^4.29 + t^4.37 + t^4.45 + t^4.63 + t^4.8 + 3*t^4.98 + t^5.06 + 4*t^5.14 + t^5.23 + t^5.31 + 3*t^5.49 + t^5.57 + t^5.65 + 2*t^5.83 + t^5.92 - 2*t^6. - t^4.29/y - t^4.29*y | detail |