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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3493 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_3\phi_1^2$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ q_1q_2\tilde{q}_2^2$ + $ M_6q_1\tilde{q}_1$ + $ M_7q_1\tilde{q}_2$ | 0.6485 | 0.852 | 0.7612 | [X:[], M:[0.9764, 1.0708, 0.9764, 0.9292, 0.7677, 0.8149, 0.7677], q:[0.7441, 0.2795], qb:[0.441, 0.4882], phi:[0.5118]] | [X:[], M:[[4], [-12], [4], [12], [-3], [-11], [-3]], q:[[1], [-5]], qb:[[10], [2]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$q_2\tilde{q}_1$, $ M_5$, $ M_7$, $ q_2\tilde{q}_2$, $ M_6$, $ M_4$, $ M_1$, $ M_3$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_5q_2\tilde{q}_1$, $ M_7q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_5^2$, $ M_5M_7$, $ M_7^2$, $ \phi_1q_1q_2$, $ M_6q_2\tilde{q}_1$, $ M_5q_2\tilde{q}_2$, $ M_7q_2\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_5M_6$, $ M_6M_7$, $ M_6q_2\tilde{q}_2$, $ M_6^2$, $ M_4q_2\tilde{q}_1$, $ M_4M_5$, $ M_4M_7$, $ \phi_1q_1\tilde{q}_1$, $ M_3q_2\tilde{q}_1$, $ M_4q_2\tilde{q}_2$, $ M_1M_5$, $ M_3M_5$, $ M_4M_6$, $ M_1M_7$, $ M_3M_7$, $ \phi_1q_1\tilde{q}_2$, $ M_3q_2\tilde{q}_2$, $ M_1M_6$, $ M_3M_6$, $ \phi_1q_2^3\tilde{q}_1$, $ M_5\phi_1q_2^2$, $ M_7\phi_1q_2^2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_4^2$, $ M_6\phi_1q_2^2$, $ M_1M_4$, $ M_3M_4$, $ M_1^2$, $ M_1M_3$, $ M_3^2$ | $M_4\phi_1q_2^2$ | -2 | t^2.16 + 3*t^2.3 + t^2.44 + t^2.79 + 2*t^2.93 + t^3.21 + t^3.84 + t^4.18 + 2*t^4.32 + 4*t^4.46 + 7*t^4.61 + 3*t^4.75 + t^4.89 + t^4.95 + 5*t^5.09 + 7*t^5.23 + 2*t^5.37 + 2*t^5.52 + t^5.58 + t^5.66 + 2*t^5.72 + t^5.86 - 2*t^6. + 2*t^6.14 + t^6.28 + t^6.34 + t^6.42 + 3*t^6.48 + 5*t^6.63 + 9*t^6.77 + 11*t^6.91 + t^6.97 + 7*t^7.05 + 3*t^7.11 + 3*t^7.19 + 6*t^7.25 + t^7.33 + 10*t^7.39 + 13*t^7.54 + 6*t^7.68 + t^7.74 + 5*t^7.82 + 4*t^7.88 + 2*t^7.96 + 5*t^8.02 + t^8.1 - 8*t^8.3 + 2*t^8.36 - t^8.44 + 4*t^8.5 + 2*t^8.59 + 5*t^8.65 + 3*t^8.73 + 3*t^8.79 + t^8.87 + t^8.93 - t^4.54/y - (2*t^6.84)/y - t^6.98/y + (2*t^7.46)/y + (5*t^7.61)/y + (3*t^7.75)/y + t^7.95/y + (6*t^8.09)/y + (9*t^8.23)/y + (3*t^8.37)/y + (3*t^8.52)/y + t^8.66/y + (2*t^8.72)/y + t^8.86/y - t^4.54*y - 2*t^6.84*y - t^6.98*y + 2*t^7.46*y + 5*t^7.61*y + 3*t^7.75*y + t^7.95*y + 6*t^8.09*y + 9*t^8.23*y + 3*t^8.37*y + 3*t^8.52*y + t^8.66*y + 2*t^8.72*y + t^8.86*y | g1^5*t^2.16 + (3*t^2.3)/g1^3 + t^2.44/g1^11 + g1^12*t^2.79 + 2*g1^4*t^2.93 + t^3.21/g1^12 + t^3.84/g1^5 + g1^18*t^4.18 + 2*g1^10*t^4.32 + 4*g1^2*t^4.46 + (7*t^4.61)/g1^6 + (3*t^4.75)/g1^14 + t^4.89/g1^22 + g1^17*t^4.95 + 5*g1^9*t^5.09 + 7*g1*t^5.23 + (2*t^5.37)/g1^7 + (2*t^5.52)/g1^15 + g1^24*t^5.58 + t^5.66/g1^23 + 2*g1^16*t^5.72 + g1^8*t^5.86 - 2*t^6. + (2*t^6.14)/g1^8 + t^6.28/g1^16 + g1^23*t^6.34 + t^6.42/g1^24 + 3*g1^15*t^6.48 + 5*g1^7*t^6.63 + (9*t^6.77)/g1 + (11*t^6.91)/g1^9 + g1^30*t^6.97 + (7*t^7.05)/g1^17 + 3*g1^22*t^7.11 + (3*t^7.19)/g1^25 + 6*g1^14*t^7.25 + t^7.33/g1^33 + 10*g1^6*t^7.39 + (13*t^7.54)/g1^2 + (6*t^7.68)/g1^10 + g1^29*t^7.74 + (5*t^7.82)/g1^18 + 4*g1^21*t^7.88 + (2*t^7.96)/g1^26 + 5*g1^13*t^8.02 + t^8.1/g1^34 - (8*t^8.3)/g1^3 + 2*g1^36*t^8.36 - t^8.44/g1^11 + 4*g1^28*t^8.5 + (2*t^8.59)/g1^19 + 5*g1^20*t^8.65 + (3*t^8.73)/g1^27 + 3*g1^12*t^8.79 + t^8.87/g1^35 + g1^4*t^8.93 - t^4.54/(g1^2*y) - (2*t^6.84)/(g1^5*y) - t^6.98/(g1^13*y) + (2*g1^2*t^7.46)/y + (5*t^7.61)/(g1^6*y) + (3*t^7.75)/(g1^14*y) + (g1^17*t^7.95)/y + (6*g1^9*t^8.09)/y + (9*g1*t^8.23)/y + (3*t^8.37)/(g1^7*y) + (3*t^8.52)/(g1^15*y) + t^8.66/(g1^23*y) + (2*g1^16*t^8.72)/y + (g1^8*t^8.86)/y - (t^4.54*y)/g1^2 - (2*t^6.84*y)/g1^5 - (t^6.98*y)/g1^13 + 2*g1^2*t^7.46*y + (5*t^7.61*y)/g1^6 + (3*t^7.75*y)/g1^14 + g1^17*t^7.95*y + 6*g1^9*t^8.09*y + 9*g1*t^8.23*y + (3*t^8.37*y)/g1^7 + (3*t^8.52*y)/g1^15 + (t^8.66*y)/g1^23 + 2*g1^16*t^8.72*y + g1^8*t^8.86*y |
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 |
---|---|---|---|---|---|---|---|---|---|
2904 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_3\phi_1^2$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ q_1q_2\tilde{q}_2^2$ + $ M_6q_1\tilde{q}_1$ | 0.6303 | 0.8194 | 0.7692 | [X:[], M:[0.9745, 1.0764, 0.9745, 0.9236, 0.7691, 0.82], q:[0.7436, 0.2818], qb:[0.4363, 0.4873], phi:[0.5127]] | t^2.15 + 2*t^2.31 + t^2.46 + t^2.77 + 2*t^2.92 + t^3.23 + t^3.69 + t^3.85 + t^4.16 + 2*t^4.31 + 3*t^4.46 + 4*t^4.61 + 2*t^4.77 + t^4.92 + t^4.93 + 4*t^5.08 + 5*t^5.23 + 2*t^5.38 + 2*t^5.54 + 3*t^5.69 + 2*t^5.85 - t^4.54/y - t^4.54*y | detail |