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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55334 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_2$ + $ M_5\phi_1\tilde{q}_1^2$ + $ M_3M_5$ + $ M_6\phi_1\tilde{q}_1\tilde{q}_2$ | 0.6707 | 0.871 | 0.7701 | [X:[], M:[1.0987, 0.7038, 1.1975, 0.7962, 0.8025, 0.6975], q:[0.75, 0.4475], qb:[0.3487, 0.4538], phi:[0.5]] | [X:[], M:[[-1], [3], [-2], [-3], [2], [-2]], q:[[0], [-2]], qb:[[-1], [3]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_6$, $ M_2$, $ M_4$, $ q_2\tilde{q}_1$, $ M_5$, $ \phi_1^2$, $ M_1$, $ q_1\tilde{q}_1$, $ M_3$, $ q_1q_2$, $ M_6^2$, $ \phi_1q_2^2$, $ M_2M_6$, $ \phi_1q_2\tilde{q}_2$, $ M_2^2$, $ \phi_1\tilde{q}_2^2$, $ M_4M_6$, $ M_6q_2\tilde{q}_1$, $ M_2M_4$, $ M_5M_6$, $ M_2q_2\tilde{q}_1$, $ M_2M_5$, $ M_4^2$, $ M_4q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ M_4M_5$, $ M_5q_2\tilde{q}_1$, $ M_5^2$, $ M_6\phi_1^2$, $ M_2\phi_1^2$, $ M_1M_6$, $ M_4\phi_1^2$, $ M_6q_1\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_1M_2$, $ M_5\phi_1^2$, $ M_2q_1\tilde{q}_1$, $ M_1M_4$, $ M_3M_6$, $ M_6q_1q_2$, $ M_4q_1\tilde{q}_1$, $ q_1q_2\tilde{q}_1^2$, $ M_2M_3$, $ M_1M_5$, $ M_2q_1q_2$, $ M_5q_1\tilde{q}_1$, $ M_3M_4$, $ M_4q_1q_2$, $ M_3q_2\tilde{q}_1$, $ q_1q_2^2\tilde{q}_1$ | $M_5q_1q_2$ | -1 | t^2.09 + t^2.11 + 2*t^2.39 + t^2.41 + t^3. + 2*t^3.3 + 2*t^3.59 + 2*t^4.18 + 2*t^4.2 + 2*t^4.22 + 2*t^4.48 + 3*t^4.5 + t^4.52 + 3*t^4.78 + 2*t^4.8 + t^4.82 + t^5.09 + t^5.11 + 4*t^5.39 + 3*t^5.41 + 5*t^5.68 + 3*t^5.7 + 3*t^5.98 - t^6. - t^6.02 + 2*t^6.28 + 2*t^6.3 + 2*t^6.32 + 2*t^6.33 + 4*t^6.57 + 8*t^6.59 + 4*t^6.61 + 2*t^6.63 + 3*t^6.87 + 7*t^6.89 + t^6.91 + t^6.93 + 4*t^7.17 + 5*t^7.18 + 2*t^7.22 + 4*t^7.48 + 3*t^7.5 + 3*t^7.52 + 9*t^7.78 + 6*t^7.8 + 3*t^7.82 + 7*t^8.07 + t^8.09 - 3*t^8.11 - t^8.13 + 7*t^8.37 + 2*t^8.43 + 3*t^8.45 + 4*t^8.67 + 7*t^8.68 + 5*t^8.7 + 4*t^8.72 + 2*t^8.74 + 6*t^8.96 + 13*t^8.98 - t^4.5/y - t^6.59/y - t^6.61/y - t^6.89/y + (2*t^7.2)/y + (2*t^7.48)/y + (3*t^7.5)/y + t^7.52/y + t^7.78/y + t^7.8/y + t^8.09/y + (2*t^8.11)/y + (5*t^8.39)/y + (4*t^8.41)/y + (5*t^8.68)/y + (3*t^8.7)/y - t^8.72/y + (3*t^8.98)/y - t^4.5*y - t^6.59*y - t^6.61*y - t^6.89*y + 2*t^7.2*y + 2*t^7.48*y + 3*t^7.5*y + t^7.52*y + t^7.78*y + t^7.8*y + t^8.09*y + 2*t^8.11*y + 5*t^8.39*y + 4*t^8.41*y + 5*t^8.68*y + 3*t^8.7*y - t^8.72*y + 3*t^8.98*y | t^2.09/g1^2 + g1^3*t^2.11 + (2*t^2.39)/g1^3 + g1^2*t^2.41 + t^3. + (2*t^3.3)/g1 + (2*t^3.59)/g1^2 + (2*t^4.18)/g1^4 + 2*g1*t^4.2 + 2*g1^6*t^4.22 + (2*t^4.48)/g1^5 + 3*t^4.5 + g1^5*t^4.52 + (3*t^4.78)/g1^6 + (2*t^4.8)/g1 + g1^4*t^4.82 + t^5.09/g1^2 + g1^3*t^5.11 + (4*t^5.39)/g1^3 + 3*g1^2*t^5.41 + (5*t^5.68)/g1^4 + 3*g1*t^5.7 + (3*t^5.98)/g1^5 - t^6. - g1^5*t^6.02 + (2*t^6.28)/g1^6 + (2*t^6.3)/g1 + 2*g1^4*t^6.32 + 2*g1^9*t^6.33 + (4*t^6.57)/g1^7 + (8*t^6.59)/g1^2 + 4*g1^3*t^6.61 + 2*g1^8*t^6.63 + (3*t^6.87)/g1^8 + (7*t^6.89)/g1^3 + g1^2*t^6.91 + g1^7*t^6.93 + (4*t^7.17)/g1^9 + (5*t^7.18)/g1^4 + 2*g1^6*t^7.22 + (4*t^7.48)/g1^5 + 3*t^7.5 + 3*g1^5*t^7.52 + (9*t^7.78)/g1^6 + (6*t^7.8)/g1 + 3*g1^4*t^7.82 + (7*t^8.07)/g1^7 + t^8.09/g1^2 - 3*g1^3*t^8.11 - g1^8*t^8.13 + (7*t^8.37)/g1^8 + 2*g1^7*t^8.43 + 3*g1^12*t^8.45 + (4*t^8.67)/g1^9 + (7*t^8.68)/g1^4 + 5*g1*t^8.7 + 4*g1^6*t^8.72 + 2*g1^11*t^8.74 + (6*t^8.96)/g1^10 + (13*t^8.98)/g1^5 - t^4.5/y - t^6.59/(g1^2*y) - (g1^3*t^6.61)/y - t^6.89/(g1^3*y) + (2*g1*t^7.2)/y + (2*t^7.48)/(g1^5*y) + (3*t^7.5)/y + (g1^5*t^7.52)/y + t^7.78/(g1^6*y) + t^7.8/(g1*y) + t^8.09/(g1^2*y) + (2*g1^3*t^8.11)/y + (5*t^8.39)/(g1^3*y) + (4*g1^2*t^8.41)/y + (5*t^8.68)/(g1^4*y) + (3*g1*t^8.7)/y - (g1^6*t^8.72)/y + (3*t^8.98)/(g1^5*y) - t^4.5*y - (t^6.59*y)/g1^2 - g1^3*t^6.61*y - (t^6.89*y)/g1^3 + 2*g1*t^7.2*y + (2*t^7.48*y)/g1^5 + 3*t^7.5*y + g1^5*t^7.52*y + (t^7.78*y)/g1^6 + (t^7.8*y)/g1 + (t^8.09*y)/g1^2 + 2*g1^3*t^8.11*y + (5*t^8.39*y)/g1^3 + 4*g1^2*t^8.41*y + (5*t^8.68*y)/g1^4 + 3*g1*t^8.7*y - g1^6*t^8.72*y + (3*t^8.98*y)/g1^5 |
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 |
---|---|---|---|---|---|---|---|---|---|
46997 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_2$ + $ M_5\phi_1\tilde{q}_1^2$ + $ M_3M_5$ | 0.6502 | 0.8314 | 0.782 | [X:[], M:[1.0997, 0.7008, 1.1994, 0.7992, 0.8006], q:[0.75, 0.4494], qb:[0.3497, 0.4508], phi:[0.5]] | t^2.1 + 3*t^2.4 + t^3. + 2*t^3.3 + 2*t^3.6 + t^3.9 + 2*t^4.2 + 2*t^4.21 + 3*t^4.5 + 3*t^4.79 + 3*t^4.8 + t^5.1 + 5*t^5.4 + 6*t^5.7 + 2*t^6. - t^4.5/y - t^4.5*y | detail |