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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2911 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_3\phi_1^2$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_6q_1\tilde{q}_1$ + $ M_6\phi_1q_2^2$ | 0.6356 | 0.8354 | 0.7609 | [X:[], M:[0.9443, 1.1671, 0.9443, 0.8329, 0.7215, 0.8329], q:[0.7361, 0.3196], qb:[0.431, 0.4019], phi:[0.5279]] | [X:[], M:[[4], [-12], [4], [12], [20], [12]], q:[[1], [-5]], qb:[[-13], [25]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_5$, $ q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ M_4$, $ M_6$, $ M_1$, $ M_3$, $ q_1\tilde{q}_2$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ M_5^2$, $ M_5q_2\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_5q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_1^2$, $ M_4M_5$, $ M_5M_6$, $ M_4q_2\tilde{q}_2$, $ M_6q_2\tilde{q}_2$, $ \phi_1q_1q_2$, $ M_4q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ M_4^2$, $ M_1M_5$, $ M_3M_5$, $ M_4M_6$, $ M_6^2$, $ \phi_1q_1\tilde{q}_2$, $ M_3q_2\tilde{q}_2$, $ \phi_1q_1\tilde{q}_1$, $ M_3q_2\tilde{q}_1$, $ M_1M_4$, $ M_3M_4$, $ M_1M_6$, $ M_3M_6$, $ M_5q_1\tilde{q}_2$, $ q_1q_2\tilde{q}_2^2$, $ M_1^2$, $ M_1M_3$, $ M_3^2$, $ M_5\phi_1q_2^2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_4q_1\tilde{q}_2$, $ M_6q_1\tilde{q}_2$, $ M_5\phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2\tilde{q}_2^2$ | $M_4\phi_1q_2^2$ | -1 | 2*t^2.16 + t^2.25 + 2*t^2.5 + 2*t^2.83 + t^3.41 + t^3.5 + t^3.75 + t^3.99 + t^4.08 + t^4.17 + 3*t^4.33 + 2*t^4.42 + t^4.5 + 4*t^4.66 + 2*t^4.75 + 7*t^5. + 2*t^5.08 + 4*t^5.33 + 2*t^5.58 + 4*t^5.67 + 3*t^5.91 - t^6. - t^6.09 + 2*t^6.16 + 5*t^6.25 + t^6.33 + t^6.42 + 6*t^6.49 + 5*t^6.58 + 2*t^6.67 + t^6.76 + 8*t^6.83 + 4*t^6.92 + 2*t^7. + 12*t^7.16 + 4*t^7.25 + t^7.41 + 12*t^7.5 + t^7.58 - t^7.67 + 4*t^7.74 + 11*t^7.83 + t^7.99 + 6*t^8.08 + 2*t^8.16 - 4*t^8.25 + 3*t^8.32 + 10*t^8.41 - t^8.5 - 3*t^8.59 + 9*t^8.66 + t^8.67 + 11*t^8.75 - 6*t^8.83 + 15*t^8.99 - t^4.58/y - t^6.75/y - t^7.08/y + t^7.33/y + t^7.42/y + (4*t^7.66)/y + (3*t^7.75)/y + (5*t^8.)/y + (3*t^8.08)/y + (4*t^8.33)/y + t^8.42/y + (2*t^8.58)/y + (4*t^8.67)/y + t^8.75/y + (3*t^8.91)/y - t^4.58*y - t^6.75*y - t^7.08*y + t^7.33*y + t^7.42*y + 4*t^7.66*y + 3*t^7.75*y + 5*t^8.*y + 3*t^8.08*y + 4*t^8.33*y + t^8.42*y + 2*t^8.58*y + 4*t^8.67*y + t^8.75*y + 3*t^8.91*y | 2*g1^20*t^2.16 + t^2.25/g1^18 + 2*g1^12*t^2.5 + 2*g1^4*t^2.83 + g1^26*t^3.41 + t^3.5/g1^12 + g1^18*t^3.75 + g1^48*t^3.99 + g1^10*t^4.08 + t^4.17/g1^28 + 3*g1^40*t^4.33 + 2*g1^2*t^4.42 + t^4.5/g1^36 + 4*g1^32*t^4.66 + (2*t^4.75)/g1^6 + 7*g1^24*t^5. + (2*t^5.08)/g1^14 + 4*g1^16*t^5.33 + 2*g1^46*t^5.58 + 4*g1^8*t^5.67 + 3*g1^38*t^5.91 - t^6. - t^6.09/g1^38 + 2*g1^68*t^6.16 + 5*g1^30*t^6.25 + t^6.33/g1^8 + t^6.42/g1^46 + 6*g1^60*t^6.49 + 5*g1^22*t^6.58 + (2*t^6.67)/g1^16 + t^6.76/g1^54 + 8*g1^52*t^6.83 + 4*g1^14*t^6.92 + (2*t^7.)/g1^24 + 12*g1^44*t^7.16 + 4*g1^6*t^7.25 + g1^74*t^7.41 + 12*g1^36*t^7.5 + t^7.58/g1^2 - t^7.67/g1^40 + 4*g1^66*t^7.74 + 11*g1^28*t^7.83 + g1^96*t^7.99 + 6*g1^58*t^8.08 + 2*g1^20*t^8.16 - (4*t^8.25)/g1^18 + 3*g1^88*t^8.32 + 10*g1^50*t^8.41 - g1^12*t^8.5 - (3*t^8.59)/g1^26 + 9*g1^80*t^8.66 + t^8.67/g1^64 + 11*g1^42*t^8.75 - 6*g1^4*t^8.83 + 15*g1^72*t^8.99 - t^4.58/(g1^2*y) - (g1^18*t^6.75)/y - (g1^10*t^7.08)/y + (g1^40*t^7.33)/y + (g1^2*t^7.42)/y + (4*g1^32*t^7.66)/y + (3*t^7.75)/(g1^6*y) + (5*g1^24*t^8.)/y + (3*t^8.08)/(g1^14*y) + (4*g1^16*t^8.33)/y + t^8.42/(g1^22*y) + (2*g1^46*t^8.58)/y + (4*g1^8*t^8.67)/y + t^8.75/(g1^30*y) + (3*g1^38*t^8.91)/y - (t^4.58*y)/g1^2 - g1^18*t^6.75*y - g1^10*t^7.08*y + g1^40*t^7.33*y + g1^2*t^7.42*y + 4*g1^32*t^7.66*y + (3*t^7.75*y)/g1^6 + 5*g1^24*t^8.*y + (3*t^8.08*y)/g1^14 + 4*g1^16*t^8.33*y + (t^8.42*y)/g1^22 + 2*g1^46*t^8.58*y + 4*g1^8*t^8.67*y + (t^8.75*y)/g1^30 + 3*g1^38*t^8.91*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 |
---|---|---|---|---|---|---|---|---|---|
1888 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_3\phi_1^2$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_6q_1\tilde{q}_1$ | 0.6371 | 0.8353 | 0.7627 | [X:[], M:[0.958, 1.1261, 0.958, 0.8739, 0.7168, 0.8009], q:[0.7395, 0.3026], qb:[0.4596, 0.4142], phi:[0.521]] | 2*t^2.15 + t^2.29 + t^2.4 + t^2.62 + 2*t^2.87 + t^3.38 + t^3.46 + t^3.71 + t^4.05 + t^4.18 + 3*t^4.3 + t^4.32 + 2*t^4.44 + 2*t^4.55 + t^4.57 + t^4.69 + 2*t^4.77 + t^4.81 + t^4.91 + 5*t^5.02 + 2*t^5.16 + t^5.24 + 2*t^5.28 + 2*t^5.5 + t^5.53 + 2*t^5.61 + 3*t^5.75 + t^5.78 + 2*t^5.86 - 2*t^6. - t^4.56/y - t^4.56*y | detail |