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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56847 | 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$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1^2$ + $ M_4^2$ + $ M_1M_6$ + $ M_7\phi_1q_1q_2$ | 0.6256 | 0.8106 | 0.7718 | [X:[], M:[1.255, 0.9597, 0.745, 1.0, 1.0202, 0.745, 0.7651], q:[0.5, 0.245], qb:[0.5403, 0.755], phi:[0.4899]] | [X:[], M:[[1], [-8], [-1], [0], [4], [-1], [3]], q:[[0], [-1]], qb:[[8], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_3$, $ M_6$, $ M_7$, $ q_2\tilde{q}_1$, $ M_2$, $ \phi_1q_2^2$, $ M_4$, $ M_5$, $ \phi_1q_2\tilde{q}_1$, $ \tilde{q}_1\tilde{q}_2$, $ M_3^2$, $ M_3M_6$, $ M_6^2$, $ \phi_1q_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_3M_7$, $ M_6M_7$, $ M_7^2$, $ \phi_1q_1\tilde{q}_1$, $ M_3q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ M_7q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1^2$, $ M_2M_3$, $ M_2M_6$, $ M_2M_7$, $ M_3\phi_1q_2^2$, $ M_6\phi_1q_2^2$, $ M_3M_4$, $ M_4M_6$, $ M_7\phi_1q_2^2$, $ M_2q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_3M_5$, $ M_5M_6$, $ M_4M_7$, $ \phi_1q_2^3\tilde{q}_1$, $ M_5M_7$, $ M_4q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_5q_2\tilde{q}_1$, $ M_2^2$, $ M_2\phi_1q_2^2$, $ M_2M_4$, $ \phi_1^2q_2^4$, $ M_2M_5$, $ M_4\phi_1q_2^2$ | $M_5\phi_1q_2^2$ | -2 | 2*t^2.23 + t^2.3 + t^2.36 + t^2.88 + t^2.94 + t^3. + t^3.06 + t^3.83 + t^3.89 + 4*t^4.47 + 2*t^4.53 + 4*t^4.59 + t^4.65 + 2*t^4.71 + t^5.11 + 3*t^5.17 + 3*t^5.23 + 4*t^5.3 + 2*t^5.36 + t^5.42 + t^5.76 + t^5.82 + t^5.88 + t^5.94 - 2*t^6. + 2*t^6.06 + 2*t^6.12 + 2*t^6.18 + t^6.24 - t^6.58 - t^6.64 + 4*t^6.7 + 3*t^6.77 + 7*t^6.83 + 4*t^6.89 + 6*t^6.95 + 2*t^7.01 + 2*t^7.07 + t^7.35 + 4*t^7.41 + 4*t^7.47 + 6*t^7.53 + 5*t^7.59 + 6*t^7.65 + 3*t^7.71 + 2*t^7.77 + t^7.99 + 2*t^8.05 + 2*t^8.11 + 2*t^8.17 - 4*t^8.23 + 3*t^8.42 + 3*t^8.48 + 3*t^8.54 + 2*t^8.6 + t^8.64 + t^8.7 + 2*t^8.76 - 4*t^8.88 - t^4.47/y - t^6.7/y - t^6.77/y - t^7.35/y + t^7.47/y + (2*t^7.53)/y + (3*t^7.59)/y + t^7.65/y + (2*t^8.11)/y + (4*t^8.17)/y + (5*t^8.23)/y + (4*t^8.3)/y + (2*t^8.36)/y + t^8.42/y + t^8.82/y + t^8.88/y + t^8.94/y - t^4.47*y - t^6.7*y - t^6.77*y - t^7.35*y + t^7.47*y + 2*t^7.53*y + 3*t^7.59*y + t^7.65*y + 2*t^8.11*y + 4*t^8.17*y + 5*t^8.23*y + 4*t^8.3*y + 2*t^8.36*y + t^8.42*y + t^8.82*y + t^8.88*y + t^8.94*y | (2*t^2.23)/g1 + g1^3*t^2.3 + g1^7*t^2.36 + t^2.88/g1^8 + t^2.94/g1^4 + t^3. + g1^4*t^3.06 + g1^5*t^3.83 + g1^9*t^3.89 + (4*t^4.47)/g1^2 + 2*g1^2*t^4.53 + 4*g1^6*t^4.59 + g1^10*t^4.65 + 2*g1^14*t^4.71 + t^5.11/g1^9 + (3*t^5.17)/g1^5 + (3*t^5.23)/g1 + 4*g1^3*t^5.3 + 2*g1^7*t^5.36 + g1^11*t^5.42 + t^5.76/g1^16 + t^5.82/g1^12 + t^5.88/g1^8 + t^5.94/g1^4 - 2*t^6. + 2*g1^4*t^6.06 + 2*g1^8*t^6.12 + 2*g1^12*t^6.18 + g1^16*t^6.24 - t^6.58/g1^11 - t^6.64/g1^7 + (4*t^6.7)/g1^3 + 3*g1*t^6.77 + 7*g1^5*t^6.83 + 4*g1^9*t^6.89 + 6*g1^13*t^6.95 + 2*g1^17*t^7.01 + 2*g1^21*t^7.07 + t^7.35/g1^10 + (4*t^7.41)/g1^6 + (4*t^7.47)/g1^2 + 6*g1^2*t^7.53 + 5*g1^6*t^7.59 + 6*g1^10*t^7.65 + 3*g1^14*t^7.71 + 2*g1^18*t^7.77 + t^7.99/g1^17 + (2*t^8.05)/g1^13 + (2*t^8.11)/g1^9 + (2*t^8.17)/g1^5 - (4*t^8.23)/g1 + 3*g1^11*t^8.42 + 3*g1^15*t^8.48 + 3*g1^19*t^8.54 + 2*g1^23*t^8.6 + t^8.64/g1^24 + t^8.7/g1^20 + (2*t^8.76)/g1^16 - (4*t^8.88)/g1^8 - t^4.47/(g1^2*y) - t^6.7/(g1^3*y) - (g1*t^6.77)/y - t^7.35/(g1^10*y) + t^7.47/(g1^2*y) + (2*g1^2*t^7.53)/y + (3*g1^6*t^7.59)/y + (g1^10*t^7.65)/y + (2*t^8.11)/(g1^9*y) + (4*t^8.17)/(g1^5*y) + (5*t^8.23)/(g1*y) + (4*g1^3*t^8.3)/y + (2*g1^7*t^8.36)/y + (g1^11*t^8.42)/y + t^8.82/(g1^12*y) + t^8.88/(g1^8*y) + t^8.94/(g1^4*y) - (t^4.47*y)/g1^2 - (t^6.7*y)/g1^3 - g1*t^6.77*y - (t^7.35*y)/g1^10 + (t^7.47*y)/g1^2 + 2*g1^2*t^7.53*y + 3*g1^6*t^7.59*y + g1^10*t^7.65*y + (2*t^8.11*y)/g1^9 + (4*t^8.17*y)/g1^5 + (5*t^8.23*y)/g1 + 4*g1^3*t^8.3*y + 2*g1^7*t^8.36*y + g1^11*t^8.42*y + (t^8.82*y)/g1^12 + (t^8.88*y)/g1^8 + (t^8.94*y)/g1^4 |
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 |
---|---|---|---|---|---|---|---|---|---|
55175 | 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$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1^2$ + $ M_4^2$ + $ M_1M_6$ | 0.6073 | 0.7772 | 0.7814 | [X:[], M:[1.2563, 0.95, 0.7437, 1.0, 1.025, 0.7437], q:[0.5, 0.2437], qb:[0.55, 0.7563], phi:[0.4875]] | 2*t^2.23 + t^2.38 + t^2.85 + t^2.92 + t^3. + t^3.08 + t^3.69 + t^3.84 + t^3.92 + 4*t^4.46 + 3*t^4.61 + 2*t^4.76 + t^5.08 + 2*t^5.16 + 2*t^5.23 + 3*t^5.31 + t^5.38 + t^5.46 + t^5.7 + t^5.77 + t^5.85 + 3*t^5.92 - 2*t^6. - t^4.46/y - t^4.46*y | detail |