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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56435 | 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_4\phi_1\tilde{q}_1^2$ + $ M_4q_2\tilde{q}_2$ + $ M_5\tilde{q}_1\tilde{q}_2$ + $ M_6q_2\tilde{q}_2$ + $ M_7\phi_1q_2\tilde{q}_1$ | 0.7222 | 0.918 | 0.7868 | [X:[], M:[0.9452, 1.0112, 1.1208, 0.7472, 0.8132, 0.7472, 0.6812], q:[0.5822, 0.4726], qb:[0.4066, 0.7802], phi:[0.4396]] | [X:[], M:[[-22], [-32], [12], [8], [-2], [8], [18]], q:[[33], [-11]], qb:[[-1], [3]], phi:[[-6]]] | 1 | {a: 154491721/213903408, c: 98181703/106951704, M1: 5986/6333, M2: 6404/6333, M3: 2366/2111, M4: 4732/6333, M5: 5150/6333, M6: 4732/6333, M7: 1438/2111, q1: 1229/2111, q2: 2993/6333, qb1: 2575/6333, qb2: 1647/2111, phi1: 928/2111} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_7$, $ M_4$, $ M_6$, $ M_5$, $ \phi_1^2$, $ M_1$, $ M_2$, $ M_3$, $ M_7^2$, $ q_1\tilde{q}_2$, $ \phi_1q_2^2$, $ M_4M_7$, $ M_6M_7$, $ \phi_1q_1\tilde{q}_1$, $ M_4^2$, $ M_4M_6$, $ M_6^2$, $ M_5M_7$, $ \phi_1q_1q_2$, $ M_4M_5$, $ M_5M_6$, $ M_7\phi_1^2$, $ \phi_1q_1^2$, $ M_5^2$, $ M_1M_7$, $ M_4\phi_1^2$, $ M_6\phi_1^2$, $ M_1M_4$, $ M_1M_6$, $ M_2M_7$, $ M_5\phi_1^2$, $ M_2M_4$, $ M_1M_5$, $ M_2M_6$, $ \phi_1^4$, $ M_3M_7$, $ M_2M_5$, $ M_1\phi_1^2$, $ M_3M_4$, $ M_3M_6$, $ M_1^2$, $ M_2\phi_1^2$, $ M_1M_2$ | . | -2 | t^2.04 + 2*t^2.24 + t^2.44 + t^2.64 + t^2.84 + t^3.03 + t^3.36 + 2*t^4.09 + t^4.15 + 3*t^4.29 + 5*t^4.48 + 3*t^4.68 + t^4.81 + 4*t^4.88 + 4*t^5.08 + 4*t^5.28 + t^5.41 + t^5.47 + 2*t^5.6 + t^5.67 + t^5.87 - 2*t^6. + t^6.07 + 2*t^6.13 + 4*t^6.33 + 2*t^6.4 + 7*t^6.53 + 10*t^6.72 + t^6.86 + 8*t^6.92 + 2*t^7.05 + 8*t^7.12 + t^7.19 + t^7.25 + 9*t^7.32 + 2*t^7.45 + 8*t^7.52 + 2*t^7.65 + 4*t^7.71 + 2*t^7.85 + 4*t^7.91 - 4*t^8.04 + 4*t^8.11 + 3*t^8.17 - 6*t^8.24 + 4*t^8.31 + 4*t^8.37 - 4*t^8.44 + 2*t^8.51 + 8*t^8.57 + t^8.7 + 11*t^8.77 - 5*t^8.84 + 3*t^8.9 + 18*t^8.97 - t^4.32/y - t^6.36/y - (2*t^6.56)/y - t^6.76/y - t^7.15/y + (3*t^7.29)/y - t^7.35/y + (3*t^7.48)/y + (3*t^7.68)/y + (4*t^7.88)/y + (6*t^8.08)/y + (4*t^8.28)/y + (2*t^8.47)/y + t^8.67/y - (3*t^8.8)/y + t^8.87/y - t^4.32*y - t^6.36*y - 2*t^6.56*y - t^6.76*y - t^7.15*y + 3*t^7.29*y - t^7.35*y + 3*t^7.48*y + 3*t^7.68*y + 4*t^7.88*y + 6*t^8.08*y + 4*t^8.28*y + 2*t^8.47*y + t^8.67*y - 3*t^8.8*y + t^8.87*y | g1^18*t^2.04 + 2*g1^8*t^2.24 + t^2.44/g1^2 + t^2.64/g1^12 + t^2.84/g1^22 + t^3.03/g1^32 + g1^12*t^3.36 + 2*g1^36*t^4.09 + t^4.15/g1^28 + 3*g1^26*t^4.29 + 5*g1^16*t^4.48 + 3*g1^6*t^4.68 + g1^60*t^4.81 + (4*t^4.88)/g1^4 + (4*t^5.08)/g1^14 + (4*t^5.28)/g1^24 + g1^30*t^5.41 + t^5.47/g1^34 + 2*g1^20*t^5.6 + t^5.67/g1^44 + t^5.87/g1^54 - 2*t^6. + t^6.07/g1^64 + 2*g1^54*t^6.13 + 4*g1^44*t^6.33 + (2*t^6.4)/g1^20 + 7*g1^34*t^6.53 + 10*g1^24*t^6.72 + g1^78*t^6.86 + 8*g1^14*t^6.92 + 2*g1^68*t^7.05 + 8*g1^4*t^7.12 + t^7.19/g1^60 + g1^58*t^7.25 + (9*t^7.32)/g1^6 + 2*g1^48*t^7.45 + (8*t^7.52)/g1^16 + 2*g1^38*t^7.65 + (4*t^7.71)/g1^26 + 2*g1^28*t^7.85 + (4*t^7.91)/g1^36 - 4*g1^18*t^8.04 + (4*t^8.11)/g1^46 + 3*g1^72*t^8.17 - 6*g1^8*t^8.24 + (4*t^8.31)/g1^56 + 4*g1^62*t^8.37 - (4*t^8.44)/g1^2 + (2*t^8.51)/g1^66 + 8*g1^52*t^8.57 + t^8.7/g1^76 + 11*g1^42*t^8.77 - (5*t^8.84)/g1^22 + t^8.9/g1^86 + 2*g1^96*t^8.9 + 18*g1^32*t^8.97 - t^4.32/(g1^6*y) - (g1^12*t^6.36)/y - (2*g1^2*t^6.56)/y - t^6.76/(g1^8*y) - t^7.15/(g1^28*y) + (3*g1^26*t^7.29)/y - t^7.35/(g1^38*y) + (3*g1^16*t^7.48)/y + (3*g1^6*t^7.68)/y + (4*t^7.88)/(g1^4*y) + (6*t^8.08)/(g1^14*y) + (4*t^8.28)/(g1^24*y) + (2*t^8.47)/(g1^34*y) + t^8.67/(g1^44*y) - (3*g1^10*t^8.8)/y + t^8.87/(g1^54*y) - (t^4.32*y)/g1^6 - g1^12*t^6.36*y - 2*g1^2*t^6.56*y - (t^6.76*y)/g1^8 - (t^7.15*y)/g1^28 + 3*g1^26*t^7.29*y - (t^7.35*y)/g1^38 + 3*g1^16*t^7.48*y + 3*g1^6*t^7.68*y + (4*t^7.88*y)/g1^4 + (6*t^8.08*y)/g1^14 + (4*t^8.28*y)/g1^24 + (2*t^8.47*y)/g1^34 + (t^8.67*y)/g1^44 - 3*g1^10*t^8.8*y + (t^8.87*y)/g1^54 |
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 |
---|---|---|---|---|---|---|---|---|---|
52636 | 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_4\phi_1\tilde{q}_1^2$ + $ M_4q_2\tilde{q}_2$ + $ M_5\tilde{q}_1\tilde{q}_2$ + $ M_6q_2\tilde{q}_2$ | 0.7015 | 0.8773 | 0.7996 | [X:[], M:[0.9436, 1.0088, 1.1217, 0.7478, 0.8131, 0.7478], q:[0.5847, 0.4718], qb:[0.4065, 0.7804], phi:[0.4392]] | 2*t^2.24 + t^2.44 + t^2.63 + t^2.83 + t^3.03 + t^3.37 + t^3.95 + t^4.1 + t^4.15 + t^4.29 + 4*t^4.49 + 2*t^4.68 + t^4.83 + 3*t^4.88 + 3*t^5.07 + 4*t^5.27 + t^5.47 + 2*t^5.61 + t^5.66 + t^5.86 - 2*t^6. - t^4.32/y - t^4.32*y | detail |