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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56334 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_3\phi_1^2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_4$ + $ M_5q_1\tilde{q}_2$ + $ M_6\phi_1q_2^2$ + $ M_7\phi_1q_1q_2$ | 0.6978 | 0.8853 | 0.7882 | [X:[], M:[1.1453, 0.9779, 1.0837, 0.8547, 0.7488, 0.7931, 0.6872], q:[0.4803, 0.3744], qb:[0.5419, 0.7709], phi:[0.4581]] | [X:[], M:[[-5], [-13], [4], [5], [-12], [14], [-3]], q:[[11], [-6]], qb:[[2], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_7$, $ M_5$, $ M_6$, $ M_4$, $ \phi_1^2$, $ M_2$, $ M_3$, $ M_1$, $ \tilde{q}_1\tilde{q}_2$, $ M_7^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_1^2$, $ M_5M_7$, $ M_6M_7$, $ \phi_1q_1\tilde{q}_1$, $ M_5^2$, $ M_5M_6$, $ M_4M_7$, $ \phi_1\tilde{q}_1^2$, $ M_6^2$, $ M_4M_5$, $ M_7\phi_1^2$, $ M_4M_6$, $ M_2M_7$, $ M_5\phi_1^2$, $ M_4^2$, $ M_6\phi_1^2$, $ M_2M_5$, $ M_2M_6$, $ M_3M_7$, $ M_4\phi_1^2$, $ M_2M_4$, $ M_3M_5$, $ M_1M_7$, $ \phi_1^4$, $ M_3M_6$, $ M_1M_5$, $ M_2\phi_1^2$, $ M_3M_4$, $ M_1M_6$, $ M_2^2$ | $M_7\tilde{q}_1\tilde{q}_2$ | 0 | t^2.06 + t^2.25 + t^2.38 + t^2.56 + t^2.75 + t^2.93 + t^3.25 + t^3.44 + t^3.94 + 2*t^4.12 + t^4.26 + t^4.31 + 2*t^4.44 + t^4.49 + 3*t^4.63 + t^4.76 + 2*t^4.81 + t^4.94 + 2*t^5. + 2*t^5.13 + t^5.18 + 3*t^5.31 + 3*t^5.5 + t^5.63 + t^5.68 + t^5.82 + t^5.87 + 3*t^6.18 + t^6.32 + 3*t^6.37 + 3*t^6.5 + t^6.55 + t^6.64 + 4*t^6.69 + t^6.74 + 3*t^6.82 + 4*t^6.87 + 4*t^7. + 3*t^7.06 + t^7.14 + 3*t^7.19 + 2*t^7.24 + t^7.32 + 5*t^7.37 + t^7.43 + 2*t^7.51 + 5*t^7.56 + 3*t^7.69 + 3*t^7.74 + 2*t^7.88 + 2*t^7.93 + t^8.01 + t^8.06 + t^8.11 + t^8.19 + 3*t^8.25 - t^8.38 + 4*t^8.43 + t^8.51 + t^8.56 + 3*t^8.62 + 2*t^8.7 + 4*t^8.75 + 2*t^8.8 + 4*t^8.88 + 2*t^8.93 + t^8.99 - t^4.37/y - t^6.44/y - t^6.62/y - t^6.75/y + (2*t^7.44)/y + (2*t^7.63)/y + (2*t^7.81)/y + t^7.94/y + (3*t^8.)/y + (2*t^8.13)/y + t^8.18/y + (4*t^8.31)/y + (2*t^8.5)/y + t^8.63/y + t^8.68/y + t^8.82/y - t^8.87/y - t^4.37*y - t^6.44*y - t^6.62*y - t^6.75*y + 2*t^7.44*y + 2*t^7.63*y + 2*t^7.81*y + t^7.94*y + 3*t^8.*y + 2*t^8.13*y + t^8.18*y + 4*t^8.31*y + 2*t^8.5*y + t^8.63*y + t^8.68*y + t^8.82*y - t^8.87*y | t^2.06/g1^3 + t^2.25/g1^12 + g1^14*t^2.38 + g1^5*t^2.56 + t^2.75/g1^4 + t^2.93/g1^13 + g1^4*t^3.25 + t^3.44/g1^5 + g1^3*t^3.94 + (2*t^4.12)/g1^6 + g1^20*t^4.26 + t^4.31/g1^15 + 2*g1^11*t^4.44 + t^4.49/g1^24 + 3*g1^2*t^4.63 + g1^28*t^4.76 + (2*t^4.81)/g1^7 + g1^19*t^4.94 + (2*t^5.)/g1^16 + 2*g1^10*t^5.13 + t^5.18/g1^25 + 3*g1*t^5.31 + (3*t^5.5)/g1^8 + g1^18*t^5.63 + t^5.68/g1^17 + g1^9*t^5.82 + t^5.87/g1^26 + (3*t^6.18)/g1^9 + g1^17*t^6.32 + (3*t^6.37)/g1^18 + 3*g1^8*t^6.5 + t^6.55/g1^27 + g1^34*t^6.64 + (4*t^6.69)/g1 + t^6.74/g1^36 + 3*g1^25*t^6.82 + (4*t^6.87)/g1^10 + 4*g1^16*t^7. + (3*t^7.06)/g1^19 + g1^42*t^7.14 + 3*g1^7*t^7.19 + (2*t^7.24)/g1^28 + g1^33*t^7.32 + (5*t^7.37)/g1^2 + t^7.43/g1^37 + 2*g1^24*t^7.51 + (5*t^7.56)/g1^11 + 3*g1^15*t^7.69 + (3*t^7.74)/g1^20 + 2*g1^6*t^7.88 + (2*t^7.93)/g1^29 + g1^32*t^8.01 + t^8.06/g1^3 + t^8.11/g1^38 + g1^23*t^8.19 + (3*t^8.25)/g1^12 - g1^14*t^8.38 + (4*t^8.43)/g1^21 + g1^40*t^8.51 + g1^5*t^8.56 + (3*t^8.62)/g1^30 + 2*g1^31*t^8.7 + (4*t^8.75)/g1^4 + (2*t^8.8)/g1^39 + 4*g1^22*t^8.88 + (2*t^8.93)/g1^13 + t^8.99/g1^48 - t^4.37/(g1^2*y) - t^6.44/(g1^5*y) - t^6.62/(g1^14*y) - (g1^12*t^6.75)/y + (2*g1^11*t^7.44)/y + (2*g1^2*t^7.63)/y + (2*t^7.81)/(g1^7*y) + (g1^19*t^7.94)/y + (3*t^8.)/(g1^16*y) + (2*g1^10*t^8.13)/y + t^8.18/(g1^25*y) + (4*g1*t^8.31)/y + (2*t^8.5)/(g1^8*y) + (g1^18*t^8.63)/y + t^8.68/(g1^17*y) + (g1^9*t^8.82)/y - t^8.87/(g1^26*y) - (t^4.37*y)/g1^2 - (t^6.44*y)/g1^5 - (t^6.62*y)/g1^14 - g1^12*t^6.75*y + 2*g1^11*t^7.44*y + 2*g1^2*t^7.63*y + (2*t^7.81*y)/g1^7 + g1^19*t^7.94*y + (3*t^8.*y)/g1^16 + 2*g1^10*t^8.13*y + (t^8.18*y)/g1^25 + 4*g1*t^8.31*y + (2*t^8.5*y)/g1^8 + g1^18*t^8.63*y + (t^8.68*y)/g1^17 + g1^9*t^8.82*y - (t^8.87*y)/g1^26 |
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 |
---|---|---|---|---|---|---|---|---|---|
50921 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_3\phi_1^2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_4$ + $ M_5q_1\tilde{q}_2$ + $ M_6\phi_1q_2^2$ | 0.6771 | 0.8451 | 0.8012 | [X:[], M:[1.1457, 0.9789, 1.0834, 0.8543, 0.7497, 0.792], q:[0.4794, 0.3749], qb:[0.5417, 0.7709], phi:[0.4583]] | t^2.25 + t^2.38 + t^2.56 + t^2.75 + t^2.94 + t^3.25 + t^3.44 + 2*t^3.94 + t^4.12 + t^4.25 + t^4.44 + t^4.5 + 2*t^4.63 + t^4.75 + t^4.81 + t^4.94 + t^5. + 2*t^5.13 + t^5.19 + 2*t^5.31 + 2*t^5.5 + t^5.63 + t^5.69 + t^5.81 + t^5.87 - t^6. - t^4.37/y - t^4.37*y | detail |