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 |
---|---|---|---|---|---|---|---|---|---|
55730 | SU2adj1nf3 | $\phi_1q_1q_2$ + $ q_2q_3$ + $ M_1\tilde{q}_1\tilde{q}_2$ + $ \phi_1^4$ | 0.694 | 0.8536 | 0.813 | [X:[], M:[0.9459], q:[0.473, 1.027, 0.973], qb:[0.527, 0.527, 0.473], phi:[0.5]] | [X:[], M:[[-1, -1, 0]], q:[[-1, -1, -1], [1, 1, 1], [-1, -1, -1]], qb:[[1, 0, 0], [0, 1, 0], [0, 0, 1]], phi:[[0, 0, 0]]] | 3 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
$M_1$, $ q_1\tilde{q}_3$, $ \phi_1^2$, $ q_1\tilde{q}_1$, $ \tilde{q}_1\tilde{q}_3$, $ q_1\tilde{q}_1$, $ \tilde{q}_1\tilde{q}_3$, $ q_3\tilde{q}_3$, $ q_1q_3$, $ \phi_1\tilde{q}_3^2$, $ q_3\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_3$, $ \phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1^2$, $ M_1q_1\tilde{q}_3$, $ q_1^2\tilde{q}_3^2$, $ M_1\phi_1^2$, $ \phi_1q_3\tilde{q}_3$, $ q_1^2\tilde{q}_1\tilde{q}_3$, $ q_1\tilde{q}_2\tilde{q}_3^2$ | $\phi_1q_3\tilde{q}_1$, $ q_1^2\tilde{q}_1^2$, $ \phi_1q_3\tilde{q}_2$, $ q_1^2\tilde{q}_1\tilde{q}_2$, $ q_1^2\tilde{q}_2^2$, $ \phi_1^2\tilde{q}_1\tilde{q}_3$, $ q_1\tilde{q}_1^2\tilde{q}_3$, $ \phi_1^2\tilde{q}_2\tilde{q}_3$, $ q_1\tilde{q}_1\tilde{q}_2\tilde{q}_3$, $ q_1\tilde{q}_2^2\tilde{q}_3$, $ \tilde{q}_1^2\tilde{q}_3^2$, $ \tilde{q}_1\tilde{q}_2\tilde{q}_3^2$, $ \tilde{q}_2^2\tilde{q}_3^2$ | 6 | 2*t^2.84 + 5*t^3. + 3*t^4.34 + 4*t^4.5 + 3*t^4.66 + 3*t^5.68 + 6*t^5.84 + 6*t^6. - 4*t^6.16 + 6*t^7.18 + 12*t^7.34 + 8*t^7.5 + 4*t^7.66 + 4*t^8.51 + 12*t^8.68 + 6*t^8.84 - t^4.5/y - t^7.34/y + t^7.66/y + t^8.68/y + (10*t^8.84)/y - t^4.5*y - t^7.34*y + t^7.66*y + t^8.68*y + 10*t^8.84*y | (2*t^2.84)/(g1*g2) + t^3. + t^3./(g1*g3) + t^3./(g2*g3) + g1*g3*t^3. + g2*g3*t^3. + t^4.34/(g1*g2) + t^4.34/(g1^2*g2^2*g3^2) + g3^2*t^4.34 + t^4.5/(g1*g3) + t^4.5/(g2*g3) + g1*g3*t^4.5 + g2*g3*t^4.5 + g1^2*t^4.66 + g1*g2*t^4.66 + g2^2*t^4.66 + (3*t^5.68)/(g1^2*g2^2) + (2*t^5.84)/(g1*g2) + t^5.84/(g1*g2^2*g3) + t^5.84/(g1^2*g2*g3) + (g3*t^5.84)/g1 + (g3*t^5.84)/g2 - 2*t^6. + t^6./(g1^2*g3^2) + t^6./(g2^2*g3^2) + t^6./(g1*g3) + t^6./(g2*g3) + g1*g3*t^6. + g2*g3*t^6. + g1^2*g3^2*t^6. + g2^2*g3^2*t^6. - (g1*t^6.16)/g3 - (g2*t^6.16)/g3 - g1^2*g2*g3*t^6.16 - g1*g2^2*g3*t^6.16 + (2*t^7.18)/(g1^2*g2^2) + (2*t^7.18)/(g1^3*g2^3*g3^2) + (2*g3^2*t^7.18)/(g1*g2) + t^7.34/(g1^2*g2^3*g3^3) + t^7.34/(g1^3*g2^2*g3^3) + (2*t^7.34)/(g1*g2^2*g3) + (2*t^7.34)/(g1^2*g2*g3) + (2*g3*t^7.34)/g1 + (2*g3*t^7.34)/g2 + g1*g3^3*t^7.34 + g2*g3^3*t^7.34 + (2*g1*t^7.5)/g2 + (2*g2*t^7.5)/g1 + t^7.5/(g1^2*g3^2) + t^7.5/(g2^2*g3^2) + g1^2*g3^2*t^7.5 + g2^2*g3^2*t^7.5 + (g1^2*t^7.66)/(g2*g3) + (g2^2*t^7.66)/(g1*g3) + g1^3*g3*t^7.66 + g2^3*g3*t^7.66 + (4*t^8.51)/(g1^3*g2^3) + (4*t^8.68)/(g1^2*g2^2) + t^8.68/(g1^4*g2^4*g3^4) + t^8.68/(g1^3*g2^3*g3^2) + t^8.68/(g1^2*g2^3*g3) + t^8.68/(g1^3*g2^2*g3) + (g3*t^8.68)/(g1*g2^2) + (g3*t^8.68)/(g1^2*g2) + (g3^2*t^8.68)/(g1*g2) + g3^4*t^8.68 - (6*t^8.84)/(g1*g2) + t^8.84/(g1^2*g2^3*g3^3) + t^8.84/(g1^3*g2^2*g3^3) + t^8.84/(g1*g2^3*g3^2) - (2*t^8.84)/(g1^2*g2^2*g3^2) + t^8.84/(g1^3*g2*g3^2) + (2*t^8.84)/(g1*g2^2*g3) + (2*t^8.84)/(g1^2*g2*g3) + (2*g3*t^8.84)/g1 + (2*g3*t^8.84)/g2 - 2*g3^2*t^8.84 + (g1*g3^2*t^8.84)/g2 + (g2*g3^2*t^8.84)/g1 + g1*g3^3*t^8.84 + g2*g3^3*t^8.84 - t^4.5/y - t^7.34/(g1*g2*y) + (g1*g2*t^7.66)/y + t^8.68/(g1^2*g2^2*y) + (2*t^8.84)/(g1*g2*y) + (2*t^8.84)/(g1*g2^2*g3*y) + (2*t^8.84)/(g1^2*g2*g3*y) + (2*g3*t^8.84)/(g1*y) + (2*g3*t^8.84)/(g2*y) - t^4.5*y - (t^7.34*y)/(g1*g2) + g1*g2*t^7.66*y + (t^8.68*y)/(g1^2*g2^2) + (2*t^8.84*y)/(g1*g2) + (2*t^8.84*y)/(g1*g2^2*g3) + (2*t^8.84*y)/(g1^2*g2*g3) + (2*g3*t^8.84*y)/g1 + (2*g3*t^8.84*y)/g2 |
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 |
---|---|---|---|---|---|---|---|---|---|
47 | SU2adj1nf2 | $\phi_1^4$ + $ M_1q_1q_2$ | 0.694 | 0.8536 | 0.813 | [X:[], M:[0.9459], q:[0.527, 0.527], qb:[0.473, 0.473], phi:[0.5]] | 2*t^2.84 + 5*t^3. + 3*t^4.34 + 4*t^4.5 + 3*t^4.66 + 3*t^5.68 + 6*t^5.84 + 6*t^6. - t^4.5/y - t^4.5*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
55671 | SU2adj1nf3 | $\phi_1q_1q_2$ + $ q_2q_3$ + $ M_1\tilde{q}_1\tilde{q}_2$ | 0.7247 | 0.8687 | 0.8342 | [X:[], M:[0.7995], q:[0.5581, 1.0211, 0.9789], qb:[0.6003, 0.6003, 0.5581], phi:[0.4208]] | t^2.4 + t^2.52 + t^3.35 + 4*t^3.48 + 3*t^4.61 + 4*t^4.74 + t^4.8 + 3*t^4.86 + t^4.92 + t^5.05 + t^5.75 + t^5.87 - 4*t^6. - t^4.26/y - t^4.26*y | detail |