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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48295 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ q_2^2\tilde{q}_1\tilde{q}_2$ + $ M_1X_1$ + $ M_3q_1\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_2^2$ + $ M_2M_5$ | 0.6977 | 0.8708 | 0.8012 | [X:[1.3333], M:[0.6667, 1.1111, 0.7695, 0.6831, 0.8889], q:[0.7778, 0.5556], qb:[0.4527, 0.4362], phi:[0.4444]] | [X:[[0]], M:[[0], [0], [1], [-2], [0]], q:[[0], [0]], qb:[[-1], [1]], phi:[[0]]] |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_4$, $ M_3$, $ M_5$, $ \phi_1^2$, $ q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ X_1$, $ \phi_1\tilde{q}_1^2$, $ M_4^2$, $ \phi_1q_2\tilde{q}_2$, $ M_3M_4$, $ \phi_1q_2\tilde{q}_1$, $ M_3^2$, $ \phi_1q_2^2$, $ M_4M_5$, $ M_4\phi_1^2$, $ M_3M_5$, $ M_3\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1q_1\tilde{q}_1$, $ M_4q_2\tilde{q}_2$, $ M_4q_2\tilde{q}_1$, $ M_3q_2\tilde{q}_2$, $ M_5^2$, $ M_5\phi_1^2$, $ \phi_1^4$, $ \phi_1q_1q_2$, $ M_3q_2\tilde{q}_1$, $ M_5q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_5q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_4q_1\tilde{q}_2$, $ M_3q_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$ | . | t^2.05 + t^2.31 + 2*t^2.67 + t^2.98 + t^3.02 + t^3.64 + 2*t^4. + t^4.05 + t^4.1 + t^4.31 + 2*t^4.36 + t^4.62 + t^4.67 + 2*t^4.72 + 2*t^4.98 + t^5.02 + t^5.07 + t^5.28 + 4*t^5.33 + t^5.64 + 2*t^5.69 + t^5.95 - 2*t^6. + 2*t^6.05 + t^6.1 + t^6.15 + 2*t^6.31 + 2*t^6.41 + 2*t^6.62 + 4*t^6.67 + 3*t^6.72 + 2*t^6.77 + t^6.93 + 2*t^6.98 + 4*t^7.02 + 2*t^7.07 + t^7.12 + 2*t^7.28 + t^7.33 + 3*t^7.38 + t^7.59 + 4*t^7.64 + 2*t^7.74 + t^7.95 + 6*t^8. - t^8.05 + 3*t^8.1 + t^8.15 + t^8.2 + t^8.26 - t^8.31 + 3*t^8.36 + t^8.41 + 2*t^8.46 + t^8.62 - 3*t^8.67 + 4*t^8.72 + 3*t^8.77 + 2*t^8.81 + 2*t^8.93 + 2*t^8.98 - t^4.33/y - t^6.38/y - t^6.64/y - t^7./y + t^7.36/y + t^7.67/y + (2*t^7.72)/y + (2*t^7.98)/y + (2*t^8.02)/y + t^8.07/y + (2*t^8.28)/y + (2*t^8.33)/y - t^8.43/y + (2*t^8.64)/y + (2*t^8.69)/y - t^4.33*y - t^6.38*y - t^6.64*y - t^7.*y + t^7.36*y + t^7.67*y + 2*t^7.72*y + 2*t^7.98*y + 2*t^8.02*y + t^8.07*y + 2*t^8.28*y + 2*t^8.33*y - t^8.43*y + 2*t^8.64*y + 2*t^8.69*y | t^2.05/g1^2 + g1*t^2.31 + 2*t^2.67 + g1*t^2.98 + t^3.02/g1 + g1*t^3.64 + 2*t^4. + t^4.05/g1^2 + t^4.1/g1^4 + g1*t^4.31 + (2*t^4.36)/g1 + g1^2*t^4.62 + t^4.67 + (2*t^4.72)/g1^2 + 2*g1*t^4.98 + t^5.02/g1 + t^5.07/g1^3 + g1^2*t^5.28 + 4*t^5.33 + g1*t^5.64 + (2*t^5.69)/g1 + g1^2*t^5.95 - 2*t^6. + (2*t^6.05)/g1^2 + t^6.1/g1^4 + t^6.15/g1^6 + 2*g1*t^6.31 + (2*t^6.41)/g1^3 + 2*g1^2*t^6.62 + 4*t^6.67 + (3*t^6.72)/g1^2 + (2*t^6.77)/g1^4 + g1^3*t^6.93 + 2*g1*t^6.98 + (4*t^7.02)/g1 + (2*t^7.07)/g1^3 + t^7.12/g1^5 + 2*g1^2*t^7.28 + t^7.33 + (3*t^7.38)/g1^2 + g1^3*t^7.59 + 4*g1*t^7.64 + (2*t^7.74)/g1^3 + g1^2*t^7.95 + 6*t^8. - t^8.05/g1^2 + (3*t^8.1)/g1^4 + t^8.15/g1^6 + t^8.2/g1^8 + g1^3*t^8.26 - g1*t^8.31 + (3*t^8.36)/g1 + t^8.41/g1^3 + (2*t^8.46)/g1^5 + g1^2*t^8.62 - 3*t^8.67 + (4*t^8.72)/g1^2 + (3*t^8.77)/g1^4 + (2*t^8.81)/g1^6 + 2*g1^3*t^8.93 + 2*g1*t^8.98 - t^4.33/y - t^6.38/(g1^2*y) - (g1*t^6.64)/y - t^7./y + t^7.36/(g1*y) + t^7.67/y + (2*t^7.72)/(g1^2*y) + (2*g1*t^7.98)/y + (2*t^8.02)/(g1*y) + t^8.07/(g1^3*y) + (2*g1^2*t^8.28)/y + (2*t^8.33)/y - t^8.43/(g1^4*y) + (2*g1*t^8.64)/y + (2*t^8.69)/(g1*y) - t^4.33*y - (t^6.38*y)/g1^2 - g1*t^6.64*y - t^7.*y + (t^7.36*y)/g1 + t^7.67*y + (2*t^7.72*y)/g1^2 + 2*g1*t^7.98*y + (2*t^8.02*y)/g1 + (t^8.07*y)/g1^3 + 2*g1^2*t^8.28*y + 2*t^8.33*y - (t^8.43*y)/g1^4 + 2*g1*t^8.64*y + (2*t^8.69*y)/g1 |
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 |
---|---|---|---|---|---|---|---|---|---|
46788 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ q_2^2\tilde{q}_1\tilde{q}_2$ + $ M_1X_1$ + $ M_3q_1\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_2^2$ | 0.6877 | 0.8539 | 0.8054 | [X:[1.3333], M:[0.6667, 1.1111, 0.7695, 0.6831], q:[0.7778, 0.5556], qb:[0.4527, 0.4362], phi:[0.4444]] | t^2.05 + t^2.31 + t^2.67 + t^2.98 + t^3.02 + t^3.33 + t^3.64 + 2*t^4. + t^4.05 + t^4.1 + t^4.31 + 2*t^4.36 + t^4.62 + t^4.67 + t^4.72 + t^4.98 + t^5.02 + t^5.07 + t^5.28 + 2*t^5.33 + t^5.38 + t^5.64 + t^5.69 + t^5.95 - t^6. - t^4.33/y - t^4.33*y | detail |