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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47264 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4\phi_1q_2^2$ + $ M_5\phi_1q_2\tilde{q}_2$ | 0.656 | 0.8685 | 0.7554 | [X:[], M:[0.9649, 0.7062, 0.8464, 0.8948, 0.7763], q:[0.7412, 0.2938], qb:[0.4825, 0.4123], phi:[0.5175]] | [X:[], M:[[4], [5], [-11], [12], [-3]], q:[[1], [-5]], qb:[[2], [10]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_2$, $ q_2\tilde{q}_2$, $ M_5$, $ q_2\tilde{q}_1$, $ M_3$, $ M_4$, $ \tilde{q}_1\tilde{q}_2$, $ M_1$, $ \phi_1^2$, $ q_1\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ M_2^2$, $ M_2q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_2M_5$, $ M_2q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ M_5q_2\tilde{q}_2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ M_2M_3$, $ M_5^2$, $ \phi_1q_1q_2$, $ M_5q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ M_3q_2\tilde{q}_2$, $ M_2M_4$, $ M_4q_2\tilde{q}_2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ M_3M_5$, $ M_3q_2\tilde{q}_1$, $ M_1M_2$, $ M_4M_5$, $ M_4q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_5\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ M_3^2$, $ M_3M_4$, $ M_1M_5$, $ M_2\phi_1^2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_2$, $ M_3\tilde{q}_1\tilde{q}_2$, $ M_4^2$, $ M_4\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_1M_3$, $ M_5\phi_1^2$, $ \phi_1^2q_2\tilde{q}_1$, $ M_1M_4$, $ M_1\tilde{q}_1\tilde{q}_2$, $ M_1^2$, $ M_4\phi_1^2$, $ M_2q_1\tilde{q}_1$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$ | $M_5q_1\tilde{q}_1$ | -1 | 2*t^2.12 + 2*t^2.33 + t^2.54 + 2*t^2.68 + t^2.89 + t^3.11 + t^3.67 + t^4.03 + 4*t^4.24 + 5*t^4.45 + 5*t^4.66 + 4*t^4.8 + 2*t^4.87 + 6*t^5.01 + t^5.08 + 6*t^5.22 + 3*t^5.37 + 2*t^5.43 + 2*t^5.58 + 3*t^5.79 - t^6. + 2*t^6.15 - t^6.21 + 8*t^6.36 + 8*t^6.57 + 2*t^6.71 + 9*t^6.78 + 8*t^6.92 + 6*t^6.99 + 13*t^7.13 + 4*t^7.2 + 14*t^7.34 + 2*t^7.41 + 6*t^7.49 + 7*t^7.55 + t^7.62 + 10*t^7.7 + 3*t^7.76 + 9*t^7.91 + 5*t^8.05 - 2*t^8.12 + 7*t^8.26 - 7*t^8.33 + 14*t^8.47 - 7*t^8.54 + 8*t^8.68 - 2*t^8.75 + 4*t^8.83 + 6*t^8.89 - t^4.55/y - t^6.67/y - t^6.88/y - t^7.09/y + (4*t^7.45)/y + (3*t^7.66)/y + (4*t^7.8)/y + (3*t^7.87)/y + (7*t^8.01)/y + (7*t^8.22)/y + t^8.37/y + (4*t^8.43)/y + (2*t^8.58)/y + t^8.64/y + (3*t^8.79)/y - t^4.55*y - t^6.67*y - t^6.88*y - t^7.09*y + 4*t^7.45*y + 3*t^7.66*y + 4*t^7.8*y + 3*t^7.87*y + 7*t^8.01*y + 7*t^8.22*y + t^8.37*y + 4*t^8.43*y + 2*t^8.58*y + t^8.64*y + 3*t^8.79*y | 2*g1^5*t^2.12 + (2*t^2.33)/g1^3 + t^2.54/g1^11 + 2*g1^12*t^2.68 + g1^4*t^2.89 + t^3.11/g1^4 + g1^3*t^3.67 + g1^18*t^4.03 + 4*g1^10*t^4.24 + 5*g1^2*t^4.45 + (5*t^4.66)/g1^6 + 4*g1^17*t^4.8 + (2*t^4.87)/g1^14 + 6*g1^9*t^5.01 + t^5.08/g1^22 + 6*g1*t^5.22 + 3*g1^24*t^5.37 + (2*t^5.43)/g1^7 + 2*g1^16*t^5.58 + 3*g1^8*t^5.79 - t^6. + 2*g1^23*t^6.15 - t^6.21/g1^8 + 8*g1^15*t^6.36 + 8*g1^7*t^6.57 + 2*g1^30*t^6.71 + (9*t^6.78)/g1 + 8*g1^22*t^6.92 + (6*t^6.99)/g1^9 + 13*g1^14*t^7.13 + (4*t^7.2)/g1^17 + 14*g1^6*t^7.34 + (2*t^7.41)/g1^25 + 6*g1^29*t^7.49 + (7*t^7.55)/g1^2 + t^7.62/g1^33 + 10*g1^21*t^7.7 + (3*t^7.76)/g1^10 + 9*g1^13*t^7.91 + 5*g1^36*t^8.05 - 2*g1^5*t^8.12 + 7*g1^28*t^8.26 - (7*t^8.33)/g1^3 + 14*g1^20*t^8.47 - (7*t^8.54)/g1^11 + 8*g1^12*t^8.68 - (2*t^8.75)/g1^19 + 4*g1^35*t^8.83 + 6*g1^4*t^8.89 - t^4.55/(g1^2*y) - (g1^3*t^6.67)/y - t^6.88/(g1^5*y) - t^7.09/(g1^13*y) + (4*g1^2*t^7.45)/y + (3*t^7.66)/(g1^6*y) + (4*g1^17*t^7.8)/y + (3*t^7.87)/(g1^14*y) + (7*g1^9*t^8.01)/y + (7*g1*t^8.22)/y + (g1^24*t^8.37)/y + (4*t^8.43)/(g1^7*y) + (2*g1^16*t^8.58)/y + t^8.64/(g1^15*y) + (3*g1^8*t^8.79)/y - (t^4.55*y)/g1^2 - g1^3*t^6.67*y - (t^6.88*y)/g1^5 - (t^7.09*y)/g1^13 + 4*g1^2*t^7.45*y + (3*t^7.66*y)/g1^6 + 4*g1^17*t^7.8*y + (3*t^7.87*y)/g1^14 + 7*g1^9*t^8.01*y + 7*g1*t^8.22*y + g1^24*t^8.37*y + (4*t^8.43*y)/g1^7 + 2*g1^16*t^8.58*y + (t^8.64*y)/g1^15 + 3*g1^8*t^8.79*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 |
---|---|---|---|---|---|---|---|---|---|
46554 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ q_1q_2\tilde{q}_1^2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4\phi_1q_2^2$ | 0.6383 | 0.8373 | 0.7623 | [X:[], M:[0.9631, 0.7039, 0.8513, 0.8894], q:[0.7408, 0.2961], qb:[0.4816, 0.4079], phi:[0.5184]] | 2*t^2.11 + t^2.33 + t^2.55 + 2*t^2.67 + t^2.89 + t^3.11 + 2*t^3.67 + t^4. + 4*t^4.22 + 3*t^4.44 + 3*t^4.67 + 4*t^4.78 + t^4.89 + 4*t^5. + t^5.11 + 5*t^5.22 + 3*t^5.34 + t^5.44 + 2*t^5.56 + 5*t^5.78 - t^6. - t^4.56/y - t^4.56*y | detail |