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 |
---|---|---|---|---|---|---|---|---|---|
4777 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1\tilde{q}_2^2$ + $ M_6\phi_1^2$ + $ M_7\phi_1q_2\tilde{q}_1$ + $ M_2M_8$ + $ q_1\tilde{q}_2$ + $ M_3X_1$ + $ M_1X_2$ | 0.4367 | 0.512 | 0.8529 | [X:[1.5895, 1.5066], M:[0.4934, 0.7119, 0.4105, 0.7947, 1.2053, 1.3974, 0.904, 1.2881], q:[1.1507, 0.3559], qb:[0.4388, 0.8493], phi:[0.3013]] | [X:[[-16], [10]], M:[[-10], [18], [16], [-8], [8], [-4], [6], [-18]], q:[[1], [9]], qb:[[-17], [-1]], phi:[[2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
$M_4$, $ M_7$, $ \phi_1q_2^2$, $ \phi_1\tilde{q}_1^2$, $ M_6$, $ M_4^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ X_1$, $ M_4M_7$, $ M_1^2q_2^2$, $ M_7^2$, $ \phi_1q_1q_2$, $ M_4\phi_1q_2^2$, $ M_4\phi_1\tilde{q}_1^2$ | $M_1M_2q_2\tilde{q}_1$ | -2 | t^2.38 + t^2.71 + t^3.04 + t^3.54 + t^4.19 + t^4.77 + t^5.1 + 2*t^5.42 + t^5.92 - 2*t^6. + t^6.08 + t^6.58 - t^6.66 + t^7.07 + 2*t^7.81 + t^8.14 + t^8.31 - 2*t^8.38 + t^8.46 - t^8.71 + t^8.96 - t^3.9/y - t^6.62/y + t^7.19/y + t^8.1/y + t^8.42/y + t^8.75/y + t^8.92/y - t^3.9*y - t^6.62*y + t^7.19*y + t^8.1*y + t^8.42*y + t^8.75*y + t^8.92*y | t^2.38/g1^8 + g1^6*t^2.71 + g1^20*t^3.04 + t^3.54/g1^32 + t^4.19/g1^4 + t^4.77/g1^16 + t^5.1/g1^2 + 2*g1^12*t^5.42 + t^5.92/g1^40 - 2*t^6. + g1^40*t^6.08 + t^6.58/g1^12 - g1^28*t^6.66 + t^7.07/g1^64 + 2*g1^4*t^7.81 + g1^18*t^8.14 + t^8.31/g1^48 - (2*t^8.38)/g1^8 + g1^32*t^8.46 - g1^6*t^8.71 + t^8.96/g1^20 - (g1^2*t^3.9)/y - (g1^8*t^6.62)/y + t^7.19/(g1^4*y) + t^8.1/(g1^2*y) + (g1^12*t^8.42)/y + (g1^26*t^8.75)/y + t^8.92/(g1^40*y) - g1^2*t^3.9*y - g1^8*t^6.62*y + (t^7.19*y)/g1^4 + (t^8.1*y)/g1^2 + g1^12*t^8.42*y + g1^26*t^8.75*y + (t^8.92*y)/g1^40 |
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 |
---|---|---|---|---|---|---|---|---|---|
2646 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1\tilde{q}_2^2$ + $ M_6\phi_1^2$ + $ M_7\phi_1q_2\tilde{q}_1$ + $ M_2M_8$ | 0.659 | 0.8115 | 0.8121 | [X:[], M:[1.0037, 0.7564, 0.9183, 0.8418, 1.1582, 1.12, 0.7182, 1.2436], q:[0.6181, 0.3782], qb:[0.4636, 0.78], phi:[0.44]] | t^2.15 + t^2.53 + t^2.75 + t^3.01 + t^3.36 + t^3.47 + t^3.59 + t^3.73 + t^4.1 + t^4.19 + 2*t^4.31 + t^4.57 + t^4.68 + t^4.91 + t^5.03 + t^5.05 + t^5.17 + 2*t^5.51 + t^5.63 + t^5.77 + 2*t^5.89 - 2*t^6. - t^4.32/y - t^4.32*y | detail |