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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1600 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_1M_4$ + $ M_5q_1\tilde{q}_1$ + $ M_6q_1q_2$ + $ M_5M_7$ + $ M_1M_8$ | 0.6841 | 0.83 | 0.8243 | [X:[], M:[1.0256, 1.1665, 0.9173, 0.9744, 0.7497, 0.6926, 1.2503, 0.9744], q:[0.7916, 0.5158], qb:[0.4587, 0.5669], phi:[0.4168]] | [X:[], M:[[7, 1], [-4, 0], [14, 0], [-7, -1], [-6, 0], [15, 1], [6, 0], [-7, -1]], q:[[-1, 0], [-14, -1]], qb:[[7, 0], [0, 1]], phi:[[2, 0]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_6$, $ M_3$, $ M_4$, $ M_8$, $ M_2$, $ M_7$, $ \phi_1\tilde{q}_1^2$, $ q_1\tilde{q}_2$, $ M_6^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_3M_6$, $ M_4M_6$, $ M_6M_8$, $ M_3^2$, $ M_2M_6$, $ M_3M_4$, $ M_3M_8$, $ M_4^2$, $ M_4M_8$, $ M_8^2$ | . | -3 | t^2.08 + t^2.75 + 2*t^2.92 + t^3.5 + t^3.75 + t^4. + t^4.08 + t^4.16 + t^4.17 + t^4.33 + t^4.34 + t^4.5 + t^4.65 + t^4.83 + 2*t^5. + t^5.5 + t^5.58 + t^5.68 + 2*t^5.85 - 3*t^6. + t^6.08 - t^6.17 + t^6.23 + t^6.25 - t^6.32 + t^6.4 + 2*t^6.42 + t^6.5 + t^6.67 + t^6.73 + t^6.75 + t^6.91 + 2*t^6.93 + t^7. + 2*t^7.08 + 2*t^7.1 + t^7.25 + 2*t^7.27 + t^7.5 + 2*t^7.58 + t^7.66 + 2*t^7.75 + t^7.83 + 2*t^7.92 + t^8. - 2*t^8.08 + t^8.15 + t^8.16 + t^8.18 - t^8.25 + t^8.26 + t^8.31 + 2*t^8.33 + t^8.35 + t^8.43 + t^8.48 + 2*t^8.5 + t^8.52 + t^8.6 + t^8.65 + t^8.69 + t^8.73 - 3*t^8.75 + 2*t^8.77 + t^8.81 + t^8.83 + t^8.84 - 6*t^8.92 + t^8.98 + t^8.99 - t^4.25/y - t^6.33/y - t^7./y - t^7.17/y + t^7.33/y + t^7.5/y + t^7.83/y + (2*t^8.)/y + t^8.17/y - t^8.41/y + t^8.58/y + (2*t^8.68)/y + t^8.83/y + t^8.85/y - t^4.25*y - t^6.33*y - t^7.*y - t^7.17*y + t^7.33*y + t^7.5*y + t^7.83*y + 2*t^8.*y + t^8.17*y - t^8.41*y + t^8.58*y + 2*t^8.68*y + t^8.83*y + t^8.85*y | g1^15*g2*t^2.08 + g1^14*t^2.75 + (2*t^2.92)/(g1^7*g2) + t^3.5/g1^4 + g1^6*t^3.75 + g1^16*t^4. + (g2*t^4.08)/g1 + g1^30*g2^2*t^4.16 + t^4.17/(g1^5*g2) + g1^9*g2*t^4.33 + t^4.34/(g1^26*g2^2) + t^4.5/g1^12 + g1^2*g2^2*t^4.65 + g1^29*g2*t^4.83 + 2*g1^8*t^5. + g1^28*t^5.5 + g1^11*g2*t^5.58 + (g1^7*t^5.68)/g2 + (2*t^5.85)/(g1^14*g2^2) - 3*t^6. + g1^31*g2*t^6.08 - t^6.17/(g1^21*g2) + g1^45*g2^3*t^6.23 + g1^10*t^6.25 - (g2*t^6.32)/g1^7 + g1^24*g2^2*t^6.4 + (2*t^6.42)/(g1^11*g2) + g1^20*t^6.5 + t^6.67/(g1*g2) + g1^17*g2^3*t^6.73 + g1^30*t^6.75 + g1^44*g2^2*t^6.91 + (2*g1^9*t^6.93)/g2 + t^7./g1^8 + 2*g1^23*g2*t^7.08 + (2*t^7.1)/(g1^12*g2^2) + g1^2*t^7.25 + (2*t^7.27)/(g1^33*g2^3) + g1^12*t^7.5 + (g2*t^7.58)/g1^5 + g1^43*g2*t^7.58 + g1^26*g2^2*t^7.66 + 2*g1^22*t^7.75 + g1^5*g2*t^7.83 + (2*g1*t^7.92)/g2 + g1^32*t^8. - 2*g1^15*g2*t^8.08 + (g2^2*t^8.15)/g1^2 + g1^46*g2^2*t^8.16 + (g1^11*t^8.18)/g2 - t^8.25/g1^6 + g1^42*t^8.26 + g1^60*g2^4*t^8.31 + 2*g1^25*g2*t^8.33 + t^8.35/(g1^10*g2^2) + (g1^21*t^8.43)/g2 + g1^39*g2^3*t^8.48 + 2*g1^4*t^8.5 + t^8.52/(g1^31*g2^3) + t^8.6/g2^2 + g1^18*g2^2*t^8.65 + t^8.69/(g1^52*g2^4) + g1*g2^3*t^8.73 - 3*g1^14*t^8.75 + (2*t^8.77)/(g1^21*g2^3) + g1^32*g2^4*t^8.81 + g1^45*g2*t^8.83 + t^8.84/(g1^38*g2^2) - (6*t^8.92)/(g1^7*g2) + g1^11*g2^3*t^8.98 + g1^59*g2^3*t^8.99 - (g1^2*t^4.25)/y - (g1^17*g2*t^6.33)/y - (g1^16*t^7.)/y - t^7.17/(g1^5*g2*y) + (g1^9*g2*t^7.33)/y + t^7.5/(g1^12*y) + (g1^29*g2*t^7.83)/y + (2*g1^8*t^8.)/y + t^8.17/(g1^13*g2*y) - (g1^32*g2^2*t^8.41)/y + (g1^11*g2*t^8.58)/y + (2*g1^7*t^8.68)/(g2*y) + (g1^21*g2*t^8.83)/y + t^8.85/(g1^14*g2^2*y) - g1^2*t^4.25*y - g1^17*g2*t^6.33*y - g1^16*t^7.*y - (t^7.17*y)/(g1^5*g2) + g1^9*g2*t^7.33*y + (t^7.5*y)/g1^12 + g1^29*g2*t^7.83*y + 2*g1^8*t^8.*y + (t^8.17*y)/(g1^13*g2) - g1^32*g2^2*t^8.41*y + g1^11*g2*t^8.58*y + (2*g1^7*t^8.68*y)/g2 + g1^21*g2*t^8.83*y + (t^8.85*y)/(g1^14*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 |
---|---|---|---|---|---|---|---|---|---|
1026 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_1M_4$ + $ M_5q_1\tilde{q}_1$ + $ M_6q_1q_2$ + $ M_5M_7$ | 0.683 | 0.8286 | 0.8242 | [X:[], M:[0.9994, 1.1648, 0.9231, 1.0006, 0.7472, 0.6698, 1.2528], q:[0.7912, 0.539], qb:[0.4615, 0.5379], phi:[0.4176]] | t^2.01 + t^2.77 + 2*t^3. + t^3.49 + t^3.76 + t^3.99 + 2*t^4.02 + 2*t^4.25 + 2*t^4.48 + t^4.49 + t^4.78 + 2*t^5.01 + t^5.5 + t^5.54 + t^5.77 - t^6. - t^4.25/y - t^4.25*y | detail |