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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56507 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_5q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_2M_5$ + $ M_6\phi_1q_1q_2$ + $ M_1M_7$ | 0.6987 | 0.8829 | 0.7914 | [X:[], M:[1.1528, 1.0455, 0.8472, 0.7561, 0.9545, 0.7024, 0.8472], q:[0.3781, 0.4691], qb:[0.5764, 0.7748], phi:[0.4504]] | [X:[], M:[[-14], [22], [14], [-30], [-22], [-12], [14]], q:[[-15], [29]], qb:[[-7], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_6$, $ M_4$, $ M_3$, $ M_7$, $ \phi_1^2$, $ M_5$, $ M_2$, $ \phi_1q_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2$, $ M_6^2$, $ \phi_1q_1\tilde{q}_1$, $ M_4M_6$, $ \phi_1q_2\tilde{q}_1$, $ M_4^2$, $ M_3M_6$, $ M_6M_7$, $ M_3M_4$, $ M_4M_7$, $ M_6\phi_1^2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_2$, $ M_5M_6$, $ M_4\phi_1^2$, $ M_3^2$, $ M_3M_7$, $ M_7^2$, $ \phi_1q_2\tilde{q}_2$, $ M_4M_5$, $ M_2M_6$, $ M_3\phi_1^2$, $ M_7\phi_1^2$, $ M_2M_4$, $ M_3M_5$, $ M_5M_7$, $ \phi_1^4$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_5\phi_1^2$, $ M_2M_3$, $ M_2M_7$, $ M_5^2$, $ M_6\phi_1q_1^2$, $ M_2\phi_1^2$, $ M_4\phi_1q_1^2$ | . | -2 | t^2.11 + t^2.27 + 2*t^2.54 + t^2.7 + t^2.86 + t^3.14 + t^3.62 + t^4.05 + t^4.17 + 2*t^4.21 + t^4.38 + t^4.49 + t^4.54 + 2*t^4.65 + 4*t^4.81 + 2*t^4.97 + 3*t^5.08 + t^5.13 + 3*t^5.24 + 3*t^5.4 + t^5.57 + t^5.68 + t^5.73 + t^5.84 + t^5.89 - 2*t^6. + 2*t^6.16 + t^6.27 + 3*t^6.32 + 3*t^6.48 + t^6.64 + 2*t^6.71 + 4*t^6.76 + t^6.8 + t^6.87 + 4*t^6.92 + t^7.03 + 5*t^7.08 + 3*t^7.19 + 3*t^7.24 + t^7.3 + 6*t^7.35 + t^7.4 - t^7.46 + 5*t^7.51 + 3*t^7.62 + 4*t^7.67 + 3*t^7.79 + 3*t^7.83 + 3*t^7.95 + t^8. + t^8.16 + t^8.22 + t^8.33 + t^8.38 + 5*t^8.43 - 4*t^8.54 + 4*t^8.59 + t^8.65 - 2*t^8.7 + 3*t^8.75 + t^8.81 + t^8.86 + t^8.91 + 2*t^8.98 - t^4.35/y - t^6.46/y - t^6.62/y - t^6.89/y - t^7.05/y + t^7.38/y + (3*t^7.65)/y + (4*t^7.81)/y + (2*t^7.97)/y + (2*t^8.08)/y + t^8.13/y + (4*t^8.24)/y + (3*t^8.4)/y + (2*t^8.68)/y + t^8.84/y - t^4.35*y - t^6.46*y - t^6.62*y - t^6.89*y - t^7.05*y + t^7.38*y + 3*t^7.65*y + 4*t^7.81*y + 2*t^7.97*y + 2*t^8.08*y + t^8.13*y + 4*t^8.24*y + 3*t^8.4*y + 2*t^8.68*y + t^8.84*y | t^2.11/g1^12 + t^2.27/g1^30 + 2*g1^14*t^2.54 + t^2.7/g1^4 + t^2.86/g1^22 + g1^22*t^3.14 + t^3.62/g1^32 + t^4.05/g1^6 + g1^56*t^4.17 + (2*t^4.21)/g1^24 + t^4.38/g1^42 + g1^20*t^4.49 + t^4.54/g1^60 + 2*g1^2*t^4.65 + (4*t^4.81)/g1^16 + (2*t^4.97)/g1^34 + 3*g1^28*t^5.08 + t^5.13/g1^52 + 3*g1^10*t^5.24 + (3*t^5.4)/g1^8 + t^5.57/g1^26 + g1^36*t^5.68 + t^5.73/g1^44 + g1^18*t^5.84 + t^5.89/g1^62 - 2*t^6. + (2*t^6.16)/g1^18 + g1^44*t^6.27 + (3*t^6.32)/g1^36 + (3*t^6.48)/g1^54 + t^6.64/g1^72 + 2*g1^70*t^6.71 + (4*t^6.76)/g1^10 + t^6.8/g1^90 + g1^52*t^6.87 + (4*t^6.92)/g1^28 + g1^34*t^7.03 + (5*t^7.08)/g1^46 + 3*g1^16*t^7.19 + (3*t^7.24)/g1^64 + g1^78*t^7.3 + (6*t^7.35)/g1^2 + t^7.4/g1^82 - g1^60*t^7.46 + (5*t^7.51)/g1^20 + 3*g1^42*t^7.62 + (4*t^7.67)/g1^38 + 3*g1^24*t^7.79 + (3*t^7.83)/g1^56 + 3*g1^6*t^7.95 + t^8./g1^74 + t^8.16/g1^92 + g1^50*t^8.22 + g1^112*t^8.33 + g1^32*t^8.38 + (5*t^8.43)/g1^48 - 4*g1^14*t^8.54 + (4*t^8.59)/g1^66 + g1^76*t^8.65 - (2*t^8.7)/g1^4 + (3*t^8.75)/g1^84 + g1^58*t^8.81 + t^8.86/g1^22 + t^8.91/g1^102 + 2*g1^40*t^8.98 - t^4.35/(g1^2*y) - t^6.46/(g1^14*y) - t^6.62/(g1^32*y) - (g1^12*t^6.89)/y - t^7.05/(g1^6*y) + t^7.38/(g1^42*y) + (3*g1^2*t^7.65)/y + (4*t^7.81)/(g1^16*y) + (2*t^7.97)/(g1^34*y) + (2*g1^28*t^8.08)/y + t^8.13/(g1^52*y) + (4*g1^10*t^8.24)/y + (3*t^8.4)/(g1^8*y) + (2*g1^36*t^8.68)/y + (g1^18*t^8.84)/y - (t^4.35*y)/g1^2 - (t^6.46*y)/g1^14 - (t^6.62*y)/g1^32 - g1^12*t^6.89*y - (t^7.05*y)/g1^6 + (t^7.38*y)/g1^42 + 3*g1^2*t^7.65*y + (4*t^7.81*y)/g1^16 + (2*t^7.97*y)/g1^34 + 2*g1^28*t^8.08*y + (t^8.13*y)/g1^52 + 4*g1^10*t^8.24*y + (3*t^8.4*y)/g1^8 + 2*g1^36*t^8.68*y + g1^18*t^8.84*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 |
---|---|---|---|---|---|---|---|---|---|
53908 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_5q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_2M_5$ + $ M_6\phi_1q_1q_2$ | 0.6856 | 0.861 | 0.7963 | [X:[], M:[1.147, 1.0546, 0.853, 0.7437, 0.9454, 0.6975], q:[0.3718, 0.4811], qb:[0.5735, 0.7752], phi:[0.4496]] | t^2.09 + t^2.23 + t^2.56 + t^2.7 + t^2.84 + t^3.16 + t^3.44 + t^3.58 + t^4.05 + 2*t^4.18 + t^4.24 + t^4.32 + t^4.46 + t^4.51 + t^4.65 + 3*t^4.79 + 2*t^4.93 + t^5.07 + t^5.12 + 2*t^5.26 + 2*t^5.39 + 2*t^5.53 + 2*t^5.67 + t^5.81 + t^5.86 - t^6. - t^4.35/y - t^4.35*y | detail |