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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2919 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_3$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_6q_1\tilde{q}_1$ + $ M_6\phi_1q_2^2$ | 0.6254 | 0.8172 | 0.7653 | [X:[], M:[0.9459, 1.1624, 1.0541, 0.8376, 0.7293, 0.8376], q:[0.7365, 0.3177], qb:[0.426, 0.4116], phi:[0.5271]] | [X:[], M:[[4], [-12], [-4], [12], [20], [12]], q:[[1], [-5]], qb:[[-13], [25]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_5$, $ q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ M_4$, $ M_6$, $ M_3$, $ \phi_1^2$, $ q_1\tilde{q}_2$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ M_5^2$, $ M_5q_2\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_5q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_1^2$, $ M_4M_5$, $ M_5M_6$, $ M_4q_2\tilde{q}_2$, $ M_6q_2\tilde{q}_2$, $ \phi_1q_1q_2$, $ M_4q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ M_4^2$, $ M_4M_6$, $ M_6^2$, $ \phi_1q_1\tilde{q}_2$, $ M_3M_5$, $ M_5\phi_1^2$, $ M_3q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_3q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_5q_1\tilde{q}_2$, $ q_1q_2\tilde{q}_2^2$, $ M_3M_4$, $ M_3M_6$, $ M_4\phi_1^2$, $ M_6\phi_1^2$, $ M_5\phi_1q_2^2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_4q_1\tilde{q}_2$, $ M_6q_1\tilde{q}_2$, $ M_5\phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2\tilde{q}_2^2$ | $M_4\phi_1q_2^2$ | -1 | 2*t^2.19 + t^2.23 + 2*t^2.51 + 2*t^3.16 + t^3.44 + t^3.49 + t^3.77 + t^4.05 + t^4.09 + t^4.14 + 3*t^4.38 + 2*t^4.42 + t^4.46 + 4*t^4.7 + 2*t^4.74 + 3*t^5.03 + 4*t^5.35 + 2*t^5.39 + 2*t^5.63 + 5*t^5.68 + 3*t^5.96 - t^6. - t^6.04 + 2*t^6.24 + 3*t^6.28 + 2*t^6.32 + t^6.37 + 6*t^6.56 + 5*t^6.61 + 4*t^6.65 + t^6.69 + 6*t^6.89 + 4*t^6.93 + 8*t^7.21 + 2*t^7.26 + t^7.5 + 10*t^7.54 + t^7.58 + t^7.62 + 4*t^7.82 + 7*t^7.86 + t^7.91 + t^8.1 + 6*t^8.14 + 2*t^8.19 - 4*t^8.23 + 3*t^8.43 + 6*t^8.47 - t^8.51 + t^8.6 + 9*t^8.75 + 9*t^8.79 + 4*t^8.84 + 2*t^8.88 + t^8.92 - t^4.58/y - t^6.77/y - t^7.09/y + t^7.38/y + (3*t^7.42)/y + (4*t^7.7)/y + t^7.74/y + t^8.03/y + t^8.07/y + (4*t^8.35)/y + (3*t^8.39)/y + (2*t^8.63)/y + (7*t^8.68)/y + t^8.72/y + (3*t^8.96)/y - t^4.58*y - t^6.77*y - t^7.09*y + t^7.38*y + 3*t^7.42*y + 4*t^7.7*y + t^7.74*y + t^8.03*y + t^8.07*y + 4*t^8.35*y + 3*t^8.39*y + 2*t^8.63*y + 7*t^8.68*y + t^8.72*y + 3*t^8.96*y | 2*g1^20*t^2.19 + t^2.23/g1^18 + 2*g1^12*t^2.51 + (2*t^3.16)/g1^4 + g1^26*t^3.44 + t^3.49/g1^12 + g1^18*t^3.77 + g1^48*t^4.05 + g1^10*t^4.09 + t^4.14/g1^28 + 3*g1^40*t^4.38 + 2*g1^2*t^4.42 + t^4.46/g1^36 + 4*g1^32*t^4.7 + (2*t^4.74)/g1^6 + 3*g1^24*t^5.03 + 4*g1^16*t^5.35 + (2*t^5.39)/g1^22 + 2*g1^46*t^5.63 + 5*g1^8*t^5.68 + 3*g1^38*t^5.96 - t^6. - t^6.04/g1^38 + 2*g1^68*t^6.24 + 3*g1^30*t^6.28 + (2*t^6.32)/g1^8 + t^6.37/g1^46 + 6*g1^60*t^6.56 + 5*g1^22*t^6.61 + (4*t^6.65)/g1^16 + t^6.69/g1^54 + 6*g1^52*t^6.89 + 4*g1^14*t^6.93 + 8*g1^44*t^7.21 + 2*g1^6*t^7.26 + g1^74*t^7.5 + 10*g1^36*t^7.54 + t^7.58/g1^2 + t^7.62/g1^40 + 4*g1^66*t^7.82 + 7*g1^28*t^7.86 + t^7.91/g1^10 + g1^96*t^8.1 + 6*g1^58*t^8.14 + 2*g1^20*t^8.19 - (4*t^8.23)/g1^18 + 3*g1^88*t^8.43 + 6*g1^50*t^8.47 - g1^12*t^8.51 + t^8.6/g1^64 + 9*g1^80*t^8.75 + 9*g1^42*t^8.79 + 4*g1^4*t^8.84 + (2*t^8.88)/g1^34 + t^8.92/g1^72 - t^4.58/(g1^2*y) - (g1^18*t^6.77)/y - (g1^10*t^7.09)/y + (g1^40*t^7.38)/y + (3*g1^2*t^7.42)/y + (4*g1^32*t^7.7)/y + t^7.74/(g1^6*y) + (g1^24*t^8.03)/y + t^8.07/(g1^14*y) + (4*g1^16*t^8.35)/y + (3*t^8.39)/(g1^22*y) + (2*g1^46*t^8.63)/y + (7*g1^8*t^8.68)/y + t^8.72/(g1^30*y) + (3*g1^38*t^8.96)/y - (t^4.58*y)/g1^2 - g1^18*t^6.77*y - g1^10*t^7.09*y + g1^40*t^7.38*y + 3*g1^2*t^7.42*y + 4*g1^32*t^7.7*y + (t^7.74*y)/g1^6 + g1^24*t^8.03*y + (t^8.07*y)/g1^14 + 4*g1^16*t^8.35*y + (3*t^8.39*y)/g1^22 + 2*g1^46*t^8.63*y + 7*g1^8*t^8.68*y + (t^8.72*y)/g1^30 + 3*g1^38*t^8.96*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 |
---|---|---|---|---|---|---|---|---|---|
1894 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_3$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_6q_1\tilde{q}_1$ | 0.6305 | 0.8225 | 0.7665 | [X:[], M:[0.9712, 1.0863, 1.0288, 0.9137, 0.7209, 0.7784], q:[0.7428, 0.286], qb:[0.4788, 0.4349], phi:[0.5144]] | 2*t^2.16 + t^2.29 + t^2.34 + t^2.74 + 2*t^3.09 + t^3.26 + t^3.53 + t^3.71 + t^4.15 + t^4.28 + 3*t^4.33 + t^4.42 + 2*t^4.46 + 2*t^4.5 + t^4.59 + t^4.63 + t^4.67 + 2*t^4.9 + t^5.04 + t^5.08 + 4*t^5.25 + 2*t^5.38 + 3*t^5.42 + t^5.48 + t^5.59 + 2*t^5.7 + 2*t^5.83 + 2*t^5.87 - 2*t^6. - t^4.54/y - t^4.54*y | detail |