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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1545 | 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_3M_7$ | 0.6522 | 0.7999 | 0.8154 | [X:[], M:[1.0397, 0.7772, 0.9784, 0.8385, 1.1615, 1.0915, 1.0216], q:[0.5717, 0.3886], qb:[0.4499, 0.7729], phi:[0.4542]] | [X:[], M:[[2, -14], [-2, -2], [-1, -15], [1, -1], [-1, 1], [0, 8], [1, 15]], q:[[-1, 15], [-1, -1]], qb:[[2, 0], [0, 2]], phi:[[0, -4]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_2$, $ M_4$, $ M_7$, $ M_1$, $ M_6$, $ M_5$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_1$, $ q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1q_2$, $ \phi_1q_1\tilde{q}_1$, $ M_2^2$, $ \phi_1q_1^2$, $ M_2M_4$, $ \phi_1q_2\tilde{q}_2$, $ M_4^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_2M_7$, $ \phi_1q_1\tilde{q}_2$, $ M_4M_7$, $ M_2M_6$, $ M_4M_6$ | . | -2 | t^2.33 + t^2.52 + t^3.06 + t^3.12 + t^3.27 + t^3.48 + t^3.69 + t^3.88 + t^4.03 + t^4.06 + t^4.24 + t^4.43 + t^4.66 + t^4.79 + t^4.85 + t^5.03 + t^5.4 + t^5.58 + t^5.61 + t^5.79 - 2*t^6. + t^6.03 + t^6.13 + t^6.21 + t^6.24 + t^6.34 + 2*t^6.39 + t^6.55 + 2*t^6.58 + 2*t^6.76 + t^6.94 + t^7. + t^7.1 + t^7.12 + t^7.13 + 2*t^7.18 + 2*t^7.31 + t^7.39 + t^7.49 + t^7.52 + t^7.55 + t^7.57 + t^7.73 + t^7.76 + t^7.86 + t^7.91 + 3*t^7.94 - t^7.97 + t^8.07 + t^8.1 + 2*t^8.12 + t^8.28 + t^8.31 - 3*t^8.33 + t^8.36 + t^8.46 + 2*t^8.49 - 3*t^8.52 + t^8.54 + t^8.57 + t^8.64 + t^8.67 - t^8.7 + t^8.73 + t^8.83 + 2*t^8.85 - t^8.88 + 2*t^8.91 - t^8.94 - t^4.36/y - t^6.69/y + t^7.24/y - t^7.48/y + t^7.85/y + t^8.03/y + t^8.4/y + t^8.45/y + t^8.58/y + t^8.61/y + t^8.63/y + t^8.79/y + t^8.82/y - t^4.36*y - t^6.69*y + t^7.24*y - t^7.48*y + t^7.85*y + t^8.03*y + t^8.4*y + t^8.45*y + t^8.58*y + t^8.61*y + t^8.63*y + t^8.79*y + t^8.82*y | t^2.33/(g1^2*g2^2) + (g1*t^2.52)/g2 + g1*g2^15*t^3.06 + (g1^2*t^3.12)/g2^14 + g2^8*t^3.27 + (g2*t^3.48)/g1 + t^3.69/(g1^2*g2^6) + (g1*t^3.88)/g2^5 + (g2^17*t^4.03)/g1 + (g1^4*t^4.06)/g2^4 + (g2^10*t^4.24)/g1^2 + g1*g2^11*t^4.43 + t^4.66/(g1^4*g2^4) + (g2^26*t^4.79)/g1^2 + t^4.85/(g1*g2^3) + (g1^2*t^5.03)/g2^2 + (g2^13*t^5.4)/g1 + g1^2*g2^14*t^5.58 + (g2^6*t^5.61)/g1^2 + g1*g2^7*t^5.79 - 2*t^6. + t^6.03/(g1^4*g2^8) + g1^2*g2^30*t^6.13 + t^6.21/(g1*g2^7) + (g1^4*t^6.24)/g2^28 + g1*g2^23*t^6.34 + (2*g1^2*t^6.39)/g2^6 + g2^16*t^6.55 + (g1^5*t^6.58)/g2^5 + (g2^8*t^6.58)/g1^4 + (2*g2^9*t^6.76)/g1 + g1^2*g2^10*t^6.94 + t^7./(g1^6*g2^6) + g2^32*t^7.1 + (g2^24*t^7.12)/g1^4 + g1^5*g2^11*t^7.13 + (g1^6*t^7.18)/g2^18 + t^7.18/(g1^3*g2^5) + (2*g2^25*t^7.31)/g1 + t^7.39/(g1^4*g2^12) + g1^2*g2^26*t^7.49 + (g2^18*t^7.52)/g1^2 + (g1^3*t^7.55)/g2^3 + t^7.57/(g1*g2^11) + (g2^11*t^7.73)/g1^3 + (g1^2*t^7.76)/g2^10 + (g2^41*t^7.86)/g1 + g2^12*t^7.91 + (g1^5*t^7.94)/g2^9 + (2*g2^4*t^7.94)/g1^4 - (g1*t^7.97)/g2^17 + (g2^34*t^8.07)/g1^2 + g1^3*g2^13*t^8.1 + (g1^8*t^8.12)/g2^8 + (g2^5*t^8.12)/g1 + (g2^27*t^8.28)/g1^3 + g1^2*g2^6*t^8.31 - (3*t^8.33)/(g1^2*g2^2) + t^8.36/(g1^6*g2^10) + g2^28*t^8.46 + g1^5*g2^7*t^8.49 + (g2^20*t^8.49)/g1^4 - (3*g1*t^8.52)/g2 + t^8.54/(g1^3*g2^9) + (g1^2*t^8.57)/g2^30 + g1^3*g2^29*t^8.64 + (g2^21*t^8.67)/g1 - g1^4*t^8.7 + t^8.73/g2^8 + (g2^43*t^8.83)/g1^3 + 2*g1^2*g2^22*t^8.85 - (g2^14*t^8.88)/g1^2 + (g1^3*t^8.91)/g2^7 + (g2^6*t^8.91)/g1^6 - t^8.94/(g1*g2^15) - t^4.36/(g2^4*y) - t^6.69/(g1^2*g2^6*y) + (g2^10*t^7.24)/(g1^2*y) - (g1^2*t^7.48)/(g2^18*y) + t^7.85/(g1*g2^3*y) + (g1^2*t^8.03)/(g2^2*y) + (g2^13*t^8.4)/(g1*y) + t^8.45/(g2^16*y) + (g1^2*g2^14*t^8.58)/y + (g2^6*t^8.61)/(g1^2*y) + (g1^3*t^8.63)/(g2^15*y) + (g1*g2^7*t^8.79)/y + t^8.82/(g1^3*g2*y) - (t^4.36*y)/g2^4 - (t^6.69*y)/(g1^2*g2^6) + (g2^10*t^7.24*y)/g1^2 - (g1^2*t^7.48*y)/g2^18 + (t^7.85*y)/(g1*g2^3) + (g1^2*t^8.03*y)/g2^2 + (g2^13*t^8.4*y)/g1 + (t^8.45*y)/g2^16 + g1^2*g2^14*t^8.58*y + (g2^6*t^8.61*y)/g1^2 + (g1^3*t^8.63*y)/g2^15 + g1*g2^7*t^8.79*y + (t^8.82*y)/(g1^3*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 |
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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 |
---|---|---|---|---|---|---|---|---|---|
984 | 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$ | 0.6579 | 0.8086 | 0.8137 | [X:[], M:[1.0037, 0.7433, 0.9002, 0.8467, 1.1533, 1.1265], q:[0.6247, 0.3716], qb:[0.4751, 0.7816], phi:[0.4367]] | t^2.23 + t^2.54 + t^2.7 + t^3.01 + t^3.38 + t^3.46 + t^3.54 + t^3.85 + t^4.16 + t^4.22 + t^4.3 + t^4.46 + t^4.61 + t^4.77 + t^4.93 + t^5.06 + t^5.08 + t^5.24 + t^5.4 + t^5.61 + t^5.71 + t^5.77 + t^5.92 - 2*t^6. - t^4.31/y - t^4.31*y | detail |