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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55948 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_2^2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_3M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_6\phi_1\tilde{q}_1^2$ | 0.6864 | 0.8594 | 0.7987 | [X:[], M:[0.9317, 1.0, 1.1632, 0.8368, 0.7211, 0.7894], q:[0.6157, 0.4526], qb:[0.3843, 0.7789], phi:[0.4421]] | [X:[], M:[[-11], [0], [-3], [3], [-1], [10]], q:[[4], [7]], qb:[[-4], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_5$, $ M_6$, $ M_4$, $ \phi_1^2$, $ M_1$, $ M_2$, $ M_3$, $ q_2\tilde{q}_2$, $ \phi_1q_2^2$, $ q_1\tilde{q}_2$, $ M_5^2$, $ \phi_1q_1\tilde{q}_1$, $ M_5M_6$, $ \phi_1q_1q_2$, $ M_4M_5$, $ M_6^2$, $ M_5\phi_1^2$, $ M_4M_6$, $ M_1M_5$, $ M_4^2$, $ M_6\phi_1^2$, $ \phi_1q_1^2$, $ M_2M_5$, $ M_1M_6$, $ M_4\phi_1^2$, $ M_1M_4$, $ \phi_1^4$, $ M_2M_6$, $ M_1\phi_1^2$, $ M_1^2$, $ M_3M_5$, $ M_2\phi_1^2$, $ M_3M_6$, $ M_5q_2\tilde{q}_2$ | . | -1 | t^2.16 + t^2.37 + t^2.51 + t^2.65 + t^2.8 + t^3. + t^3.49 + t^3.69 + t^4.04 + t^4.18 + 2*t^4.33 + 2*t^4.53 + t^4.67 + t^4.74 + t^4.82 + t^4.88 + t^4.96 + 3*t^5.02 + 3*t^5.16 + t^5.31 + t^5.37 + t^5.45 + t^5.59 + 2*t^5.65 + 2*t^5.86 - t^6. + t^6.06 + t^6.2 + t^6.28 + t^6.35 + t^6.41 + 2*t^6.49 + 2*t^6.55 - t^6.63 + 4*t^6.69 + t^6.84 + 2*t^6.9 + 2*t^6.98 + 2*t^7.04 + t^7.1 + t^7.12 + 4*t^7.18 + t^7.25 + 2*t^7.33 + 3*t^7.39 + t^7.47 + 4*t^7.53 + t^7.61 + 2*t^7.67 + 2*t^7.74 + t^7.75 + 4*t^7.82 + 2*t^7.96 + 3*t^8.02 + t^8.08 + t^8.1 - 3*t^8.16 + 3*t^8.23 + t^8.24 - t^8.37 + t^8.39 + t^8.43 + t^8.45 + 2*t^8.57 + t^8.65 + 3*t^8.72 + t^8.78 - 3*t^8.8 + 2*t^8.86 + 2*t^8.92 - t^4.33/y - t^6.49/y - t^6.69/y - t^6.98/y - t^7.12/y + (2*t^7.53)/y + (2*t^7.67)/y + t^7.82/y + t^7.88/y + (2*t^7.96)/y + t^8.02/y + (4*t^8.16)/y + t^8.31/y + t^8.37/y + t^8.45/y + t^8.51/y + t^8.65/y + t^8.8/y + t^8.86/y - t^4.33*y - t^6.49*y - t^6.69*y - t^6.98*y - t^7.12*y + 2*t^7.53*y + 2*t^7.67*y + t^7.82*y + t^7.88*y + 2*t^7.96*y + t^8.02*y + 4*t^8.16*y + t^8.31*y + t^8.37*y + t^8.45*y + t^8.51*y + t^8.65*y + t^8.8*y + t^8.86*y | t^2.16/g1 + g1^10*t^2.37 + g1^3*t^2.51 + t^2.65/g1^4 + t^2.8/g1^11 + t^3. + t^3.49/g1^3 + g1^8*t^3.69 + g1^12*t^4.04 + g1^5*t^4.18 + (2*t^4.33)/g1^2 + 2*g1^9*t^4.53 + g1^2*t^4.67 + g1^20*t^4.74 + t^4.82/g1^5 + g1^13*t^4.88 + t^4.96/g1^12 + 3*g1^6*t^5.02 + (3*t^5.16)/g1 + t^5.31/g1^8 + g1^10*t^5.37 + t^5.45/g1^15 + t^5.59/g1^22 + (2*t^5.65)/g1^4 + 2*g1^7*t^5.86 - t^6. + g1^18*t^6.06 + g1^11*t^6.2 + t^6.28/g1^14 + g1^4*t^6.35 + g1^22*t^6.41 + (2*t^6.49)/g1^3 + 2*g1^15*t^6.55 - t^6.63/g1^10 + 4*g1^8*t^6.69 + g1*t^6.84 + 2*g1^19*t^6.9 + (2*t^6.98)/g1^6 + 2*g1^12*t^7.04 + g1^30*t^7.1 + t^7.12/g1^13 + 4*g1^5*t^7.18 + g1^23*t^7.25 + (2*t^7.33)/g1^2 + 3*g1^16*t^7.39 + t^7.47/g1^9 + 4*g1^9*t^7.53 + t^7.61/g1^16 + 2*g1^2*t^7.67 + 2*g1^20*t^7.74 + t^7.75/g1^23 + (4*t^7.82)/g1^5 + (2*t^7.96)/g1^12 + 3*g1^6*t^8.02 + g1^24*t^8.08 + t^8.1/g1^19 - (3*t^8.16)/g1 + 3*g1^17*t^8.23 + t^8.24/g1^26 - g1^10*t^8.37 + t^8.39/g1^33 + g1^28*t^8.43 + t^8.45/g1^15 + 2*g1^21*t^8.57 + t^8.65/g1^4 + 3*g1^14*t^8.72 + g1^32*t^8.78 - (3*t^8.8)/g1^11 + 2*g1^7*t^8.86 + 2*g1^25*t^8.92 - t^4.33/(g1^2*y) - t^6.49/(g1^3*y) - (g1^8*t^6.69)/y - t^6.98/(g1^6*y) - t^7.12/(g1^13*y) + (2*g1^9*t^7.53)/y + (2*g1^2*t^7.67)/y + t^7.82/(g1^5*y) + (g1^13*t^7.88)/y + (2*t^7.96)/(g1^12*y) + (g1^6*t^8.02)/y + (4*t^8.16)/(g1*y) + t^8.31/(g1^8*y) + (g1^10*t^8.37)/y + t^8.45/(g1^15*y) + (g1^3*t^8.51)/y + t^8.65/(g1^4*y) + t^8.8/(g1^11*y) + (g1^7*t^8.86)/y - (t^4.33*y)/g1^2 - (t^6.49*y)/g1^3 - g1^8*t^6.69*y - (t^6.98*y)/g1^6 - (t^7.12*y)/g1^13 + 2*g1^9*t^7.53*y + 2*g1^2*t^7.67*y + (t^7.82*y)/g1^5 + g1^13*t^7.88*y + (2*t^7.96*y)/g1^12 + g1^6*t^8.02*y + (4*t^8.16*y)/g1 + (t^8.31*y)/g1^8 + g1^10*t^8.37*y + (t^8.45*y)/g1^15 + g1^3*t^8.51*y + (t^8.65*y)/g1^4 + (t^8.8*y)/g1^11 + g1^7*t^8.86*y |
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 |
---|---|---|---|---|---|---|---|---|---|
48196 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_2^2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_3M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ | 0.6702 | 0.8305 | 0.807 | [X:[], M:[0.8959, 1.0, 1.1534, 0.8466, 0.7178], q:[0.6288, 0.4754], qb:[0.3712, 0.7822], phi:[0.4356]] | t^2.15 + t^2.54 + t^2.61 + t^2.69 + t^3. + t^3.46 + t^3.53 + t^3.77 + t^4.16 + t^4.23 + 2*t^4.31 + t^4.62 + t^4.69 + t^4.77 + t^4.84 + 2*t^5.08 + 2*t^5.15 + t^5.23 + t^5.3 + t^5.38 + 2*t^5.61 + t^5.69 + t^5.93 - t^6. - t^4.31/y - t^4.31*y | detail |