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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46756 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_3M_4$ + $ \phi_1q_1q_2$ + $ M_1X_1$ + $ M_3M_5$ | 0.6348 | 0.784 | 0.8097 | [X:[1.6126], M:[0.3874, 0.7117, 1.1621, 0.8379, 0.8379], q:[0.8536, 0.759], qb:[0.4347, 0.4032], phi:[0.3874]] | [X:[[0, 1]], M:[[0, -1], [0, -7], [0, -3], [0, 3], [0, 3]], q:[[1, 4], [-1, -3]], qb:[[-1, 3], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_2$, $ \phi_1^2$, $ M_4$, $ M_5$, $ q_2\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ M_2^2$, $ M_2\phi_1^2$, $ M_2M_4$, $ M_2M_5$, $ \phi_1^4$, $ \phi_1q_2\tilde{q}_2$, $ M_4\phi_1^2$, $ M_5\phi_1^2$, $ X_1$, $ M_4^2$, $ M_4M_5$, $ M_5^2$, $ \phi_1q_1\tilde{q}_1$, $ M_2\phi_1\tilde{q}_2^2$, $ \phi_1q_2^2$, $ M_2q_2\tilde{q}_1$, $ \phi_1^3\tilde{q}_2^2$, $ \phi_1^2q_2\tilde{q}_1$, $ M_2\phi_1\tilde{q}_1^2$ | $\phi_1^3\tilde{q}_1\tilde{q}_2$ | -2 | t^2.13 + t^2.32 + 2*t^2.51 + 2*t^3.58 + t^3.68 + 2*t^3.77 + t^4.27 + t^4.46 + 3*t^4.65 + 3*t^4.84 + 3*t^5.03 + 2*t^5.72 + 2*t^5.91 - 2*t^6. + 4*t^6.09 + t^6.19 + 4*t^6.28 + t^6.4 + t^6.59 + 3*t^6.78 + 3*t^6.97 - 2*t^7.07 + 6*t^7.16 - 2*t^7.26 + 6*t^7.35 + 6*t^7.54 + 2*t^7.85 + 2*t^8.04 - 3*t^8.13 + 4*t^8.23 - 3*t^8.32 + 4*t^8.42 - 6*t^8.51 + t^8.54 + 6*t^8.61 + t^8.73 + 6*t^8.8 + 3*t^8.92 - t^4.16/y - t^6.3/y - t^6.49/y - t^6.68/y + t^7.46/y + (3*t^7.65)/y + (3*t^7.84)/y + (2*t^8.03)/y - t^8.43/y - t^8.62/y + (2*t^8.72)/y - t^8.81/y + (4*t^8.91)/y - t^4.16*y - t^6.3*y - t^6.49*y - t^6.68*y + t^7.46*y + 3*t^7.65*y + 3*t^7.84*y + 2*t^8.03*y - t^8.43*y - t^8.62*y + 2*t^8.72*y - t^8.81*y + 4*t^8.91*y | t^2.13/g2^7 + t^2.32/g2^2 + 2*g2^3*t^2.51 + t^3.58/g1^2 + (g1^2*t^3.58)/g2 + g2^2*t^3.68 + g1^2*g2^4*t^3.77 + (g2^5*t^3.77)/g1^2 + t^4.27/g2^14 + t^4.46/g2^9 + (3*t^4.65)/g2^4 + 3*g2*t^4.84 + 3*g2^6*t^5.03 + (g1^2*t^5.72)/g2^8 + t^5.72/(g1^2*g2^7) + (g1^2*t^5.91)/g2^3 + t^5.91/(g1^2*g2^2) - 2*t^6. + 2*g1^2*g2^2*t^6.09 + (2*g2^3*t^6.09)/g1^2 + g2^5*t^6.19 + 2*g1^2*g2^7*t^6.28 + (2*g2^8*t^6.28)/g1^2 + t^6.4/g2^21 + t^6.59/g2^16 + (3*t^6.78)/g2^11 + (3*t^6.97)/g2^6 - (g1^2*t^7.07)/g2^4 - t^7.07/(g1^2*g2^3) + t^7.16/g1^4 + (g1^4*t^7.16)/g2^2 + (4*t^7.16)/g2 - g1^2*g2*t^7.26 - (g2^2*t^7.26)/g1^2 + g1^4*g2^3*t^7.35 + 4*g2^4*t^7.35 + (g2^5*t^7.35)/g1^4 + g1^4*g2^8*t^7.54 + 4*g2^9*t^7.54 + (g2^10*t^7.54)/g1^4 + (g1^2*t^7.85)/g2^15 + t^7.85/(g1^2*g2^14) + (g1^2*t^8.04)/g2^10 + t^8.04/(g1^2*g2^9) - (3*t^8.13)/g2^7 + (2*g1^2*t^8.23)/g2^5 + (2*t^8.23)/(g1^2*g2^4) - (3*t^8.32)/g2^2 + 2*g1^2*t^8.42 + (2*g2*t^8.42)/g1^2 - 6*g2^3*t^8.51 + t^8.54/g2^28 + 3*g1^2*g2^5*t^8.61 + (3*g2^6*t^8.61)/g1^2 + t^8.73/g2^23 + 3*g1^2*g2^10*t^8.8 + (3*g2^11*t^8.8)/g1^2 + (3*t^8.92)/g2^18 - t^4.16/(g2*y) - t^6.3/(g2^8*y) - t^6.49/(g2^3*y) - (g2^2*t^6.68)/y + t^7.46/(g2^9*y) + (3*t^7.65)/(g2^4*y) + (3*g2*t^7.84)/y + (2*g2^6*t^8.03)/y - t^8.43/(g2^15*y) - t^8.62/(g2^10*y) + (g1^2*t^8.72)/(g2^8*y) + t^8.72/(g1^2*g2^7*y) - t^8.81/(g2^5*y) + (2*g1^2*t^8.91)/(g2^3*y) + (2*t^8.91)/(g1^2*g2^2*y) - (t^4.16*y)/g2 - (t^6.3*y)/g2^8 - (t^6.49*y)/g2^3 - g2^2*t^6.68*y + (t^7.46*y)/g2^9 + (3*t^7.65*y)/g2^4 + 3*g2*t^7.84*y + 2*g2^6*t^8.03*y - (t^8.43*y)/g2^15 - (t^8.62*y)/g2^10 + (g1^2*t^8.72*y)/g2^8 + (t^8.72*y)/(g1^2*g2^7) - (t^8.81*y)/g2^5 + (2*g1^2*t^8.91*y)/g2^3 + (2*t^8.91*y)/(g1^2*g2^2) |
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 |
---|---|---|---|---|---|---|---|---|---|
46187 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_3M_4$ + $ \phi_1q_1q_2$ + $ M_1X_1$ | 0.6212 | 0.7607 | 0.8166 | [X:[1.6162], M:[0.3838, 0.6865, 1.1513, 0.8487], q:[0.8689, 0.7473], qb:[0.4446, 0.4041], phi:[0.3838]] | t^2.06 + t^2.3 + t^2.55 + t^3.45 + 2*t^3.58 + t^3.7 + 2*t^3.82 + t^4.12 + t^4.36 + 2*t^4.61 + 2*t^4.85 + t^5.09 + t^5.51 + 2*t^5.64 + t^5.76 + 2*t^5.88 - t^6. - t^4.15/y - t^4.15*y | detail |