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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56598 | 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_2\phi_1^2$ + $ M_5\tilde{q}_1\tilde{q}_2$ + $ M_6\phi_1q_1^2$ + $ M_2M_7$ + $ M_6q_2\tilde{q}_1$ | 0.7194 | 0.9002 | 0.7992 | [X:[], M:[0.9785, 1.087, 1.0215, 0.739, 0.8475, 0.8045, 0.913], q:[0.3695, 0.652], qb:[0.5435, 0.609], phi:[0.4565]] | [X:[], M:[[11], [2], [-11], [-6], [-15], [7], [-2]], q:[[-3], [-8]], qb:[[1], [14]], phi:[[-1]]] | 1 | {a: 1723997/2396304, c: 1078525/1198152, M1: 1136/1161, M2: 1262/1161, M3: 1186/1161, M4: 286/387, M5: 328/387, M6: 934/1161, M7: 1060/1161, q1: 143/387, q2: 757/1161, qb1: 631/1161, qb2: 707/1161, phi1: 530/1161} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_4$, $ M_6$, $ M_5$, $ M_7$, $ \phi_1^2$, $ M_1$, $ M_3$, $ q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_4^2$, $ \phi_1q_1q_2$, $ M_4M_6$, $ \phi_1\tilde{q}_1^2$, $ M_4M_5$, $ M_6^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_5M_6$, $ M_4M_7$, $ M_4\phi_1^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ M_5^2$, $ M_1M_4$, $ M_6M_7$, $ M_6\phi_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_3M_4$, $ M_5M_7$, $ M_5\phi_1^2$, $ \phi_1q_2^2$, $ M_1M_6$, $ M_1M_5$, $ M_3M_6$, $ M_7^2$, $ M_7\phi_1^2$, $ \phi_1^4$, $ M_3M_5$, $ M_1M_7$, $ M_1\phi_1^2$, $ M_3M_7$, $ M_3\phi_1^2$, $ M_4q_2\tilde{q}_1$ | . | -2 | t^2.22 + t^2.41 + t^2.54 + 2*t^2.74 + t^2.94 + t^3.06 + t^3.59 + t^4.11 + t^4.3 + 2*t^4.43 + 2*t^4.63 + t^4.76 + 2*t^4.83 + 4*t^4.96 + t^5.02 + t^5.09 + 3*t^5.15 + 3*t^5.28 + t^5.35 + 4*t^5.48 + t^5.61 + t^5.67 + 2*t^5.8 - 2*t^6. + t^6.13 - t^6.2 + 2*t^6.33 + 3*t^6.65 + 3*t^6.85 + 2*t^6.98 + 4*t^7.04 + 7*t^7.17 + 3*t^7.24 + t^7.3 + 5*t^7.37 + t^7.44 + 5*t^7.5 + 4*t^7.57 + t^7.63 + 7*t^7.7 + 3*t^7.76 + 3*t^7.82 + 3*t^7.89 + t^7.96 + 7*t^8.02 + t^8.15 + t^8.22 - t^8.28 + 3*t^8.35 - 3*t^8.41 + t^8.54 - t^8.61 + t^8.67 - 6*t^8.74 + 4*t^8.87 - 4*t^8.94 - t^4.37/y - t^6.59/y - t^6.78/y - t^6.91/y - t^7.11/y + (2*t^7.63)/y + t^7.76/y + t^7.83/y + (4*t^7.96)/y + (4*t^8.15)/y + (3*t^8.28)/y + t^8.35/y + (3*t^8.48)/y + t^8.61/y + (2*t^8.67)/y + (2*t^8.8)/y - t^4.37*y - t^6.59*y - t^6.78*y - t^6.91*y - t^7.11*y + 2*t^7.63*y + t^7.76*y + t^7.83*y + 4*t^7.96*y + 4*t^8.15*y + 3*t^8.28*y + t^8.35*y + 3*t^8.48*y + t^8.61*y + 2*t^8.67*y + 2*t^8.8*y | t^2.22/g1^6 + g1^7*t^2.41 + t^2.54/g1^15 + (2*t^2.74)/g1^2 + g1^11*t^2.94 + t^3.06/g1^11 + t^3.59/g1^7 + t^4.11/g1^3 + g1^10*t^4.3 + (2*t^4.43)/g1^12 + 2*g1*t^4.63 + t^4.76/g1^21 + 2*g1^14*t^4.83 + (4*t^4.96)/g1^8 + g1^27*t^5.02 + t^5.09/g1^30 + 3*g1^5*t^5.15 + (3*t^5.28)/g1^17 + g1^18*t^5.35 + (4*t^5.48)/g1^4 + t^5.61/g1^26 + g1^9*t^5.67 + (2*t^5.8)/g1^13 - 2*t^6. + t^6.13/g1^22 - g1^13*t^6.2 + (2*t^6.33)/g1^9 + (3*t^6.65)/g1^18 + (3*t^6.85)/g1^5 + (2*t^6.98)/g1^27 + 4*g1^8*t^7.04 + (7*t^7.17)/g1^14 + 3*g1^21*t^7.24 + t^7.3/g1^36 + (5*t^7.37)/g1 + g1^34*t^7.44 + (5*t^7.5)/g1^23 + 4*g1^12*t^7.57 + t^7.63/g1^45 + (7*t^7.7)/g1^10 + 3*g1^25*t^7.76 + (3*t^7.82)/g1^32 + 3*g1^3*t^7.89 + g1^38*t^7.96 + (7*t^8.02)/g1^19 + t^8.15/g1^41 + t^8.22/g1^6 - g1^29*t^8.28 + (3*t^8.35)/g1^28 - 3*g1^7*t^8.41 + t^8.54/g1^15 - g1^20*t^8.61 + t^8.67/g1^37 - (6*t^8.74)/g1^2 + (4*t^8.87)/g1^24 - 4*g1^11*t^8.94 - t^4.37/(g1*y) - t^6.59/(g1^7*y) - (g1^6*t^6.78)/y - t^6.91/(g1^16*y) - t^7.11/(g1^3*y) + (2*g1*t^7.63)/y + t^7.76/(g1^21*y) + (g1^14*t^7.83)/y + (4*t^7.96)/(g1^8*y) + (4*g1^5*t^8.15)/y + (3*t^8.28)/(g1^17*y) + (g1^18*t^8.35)/y + (3*t^8.48)/(g1^4*y) + t^8.61/(g1^26*y) + (2*g1^9*t^8.67)/y + (2*t^8.8)/(g1^13*y) - (t^4.37*y)/g1 - (t^6.59*y)/g1^7 - g1^6*t^6.78*y - (t^6.91*y)/g1^16 - (t^7.11*y)/g1^3 + 2*g1*t^7.63*y + (t^7.76*y)/g1^21 + g1^14*t^7.83*y + (4*t^7.96*y)/g1^8 + 4*g1^5*t^8.15*y + (3*t^8.28*y)/g1^17 + g1^18*t^8.35*y + (3*t^8.48*y)/g1^4 + (t^8.61*y)/g1^26 + 2*g1^9*t^8.67*y + (2*t^8.8*y)/g1^13 |
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 |
---|---|---|---|---|---|---|---|---|---|
54585 | 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_2\phi_1^2$ + $ M_5\tilde{q}_1\tilde{q}_2$ + $ M_6\phi_1q_1^2$ + $ M_2M_7$ | 0.735 | 0.921 | 0.7981 | [X:[], M:[1.0277, 1.0526, 0.9723, 0.8422, 0.867, 0.6841, 0.9474], q:[0.4211, 0.5512], qb:[0.5263, 0.6066], phi:[0.4737]] | t^2.05 + t^2.53 + t^2.6 + 2*t^2.84 + t^2.92 + t^3.08 + t^3.23 + t^4.1 + t^4.26 + t^4.34 + t^4.5 + 2*t^4.58 + 2*t^4.65 + t^4.73 + t^4.82 + 3*t^4.89 + t^4.97 + t^5.05 + t^5.06 + t^5.13 + t^5.14 + t^5.2 + t^5.28 + 2*t^5.37 + 2*t^5.44 + t^5.52 + 3*t^5.68 + 2*t^5.76 + t^5.83 + t^5.93 - 3*t^6. - t^4.42/y - t^4.42*y | detail |