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 |
|---|---|---|---|---|---|---|---|---|---|
| 1882 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_2\phi_1^2$ + $ q_2^2\tilde{q}_1^2$ + $ M_2M_3$ + $ M_4\phi_1\tilde{q}_2^2$ + $ M_5q_1\tilde{q}_2$ | 0.7185 | 0.9121 | 0.7877 | [X:[], M:[0.6738, 1.1087, 0.8913, 0.6738, 0.7826], q:[0.7772, 0.549], qb:[0.451, 0.4403], phi:[0.4456]] | [X:[], M:[[-12], [4], [-4], [-12], [-8]], q:[[1], [11]], qb:[[-11], [7]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ M_4$, $ M_5$, $ M_3$, $ \phi_1^2$, $ q_2\tilde{q}_2$, $ q_2\tilde{q}_1$, $ q_1\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1^2$, $ M_1M_4$, $ M_4^2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ M_1M_5$, $ M_4M_5$, $ \phi_1q_2^2$, $ M_1M_3$, $ M_3M_4$, $ M_5^2$, $ M_1\phi_1^2$, $ M_4\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ M_4q_2\tilde{q}_2$, $ M_3M_5$, $ M_5\phi_1^2$, $ \phi_1q_1\tilde{q}_1$, $ M_4q_2\tilde{q}_1$, $ \phi_1q_1q_2$, $ M_5q_2\tilde{q}_2$, $ M_3^2$, $ M_3\phi_1^2$, $ \phi_1^4$, $ M_5q_2\tilde{q}_1$, $ M_3q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_3q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_4q_1\tilde{q}_1$, $ q_2^2\tilde{q}_2^2$ | . | -2 | 2*t^2.02 + t^2.35 + 2*t^2.67 + t^2.97 + t^3. + t^3.68 + t^4.01 + 4*t^4.04 + t^4.3 + t^4.34 + 2*t^4.37 + t^4.63 + 5*t^4.7 + 2*t^4.99 + 4*t^5.02 + t^5.32 + 4*t^5.35 + 2*t^5.64 + t^5.67 + t^5.71 + t^5.94 - 2*t^6. + 2*t^6.03 + 6*t^6.06 - t^6.29 + 4*t^6.36 + 4*t^6.39 + 2*t^6.65 + 3*t^6.68 + 10*t^6.72 + 2*t^6.98 + 4*t^7.01 + 8*t^7.04 + t^7.27 + t^7.3 + 9*t^7.37 + t^7.6 - t^7.63 + 2*t^7.66 + 6*t^7.7 + 2*t^7.73 + t^7.99 + t^8.02 + 3*t^8.05 + 9*t^8.09 - 2*t^8.35 + 6*t^8.38 + 6*t^8.41 + 2*t^8.61 - 2*t^8.64 - 4*t^8.67 + 6*t^8.71 + 16*t^8.74 + t^8.9 + t^8.94 - 4*t^8.97 - t^4.34/y - (2*t^6.36)/y - t^6.68/y - t^7.01/y + t^7.04/y + (2*t^7.37)/y + t^7.66/y + (4*t^7.7)/y + (3*t^7.99)/y + (4*t^8.02)/y + (3*t^8.32)/y + (2*t^8.35)/y - (3*t^8.38)/y + (2*t^8.64)/y + (2*t^8.67)/y + t^8.97/y - t^4.34*y - 2*t^6.36*y - t^6.68*y - t^7.01*y + t^7.04*y + 2*t^7.37*y + t^7.66*y + 4*t^7.7*y + 3*t^7.99*y + 4*t^8.02*y + 3*t^8.32*y + 2*t^8.35*y - 3*t^8.38*y + 2*t^8.64*y + 2*t^8.67*y + t^8.97*y | (2*t^2.02)/g1^12 + t^2.35/g1^8 + (2*t^2.67)/g1^4 + g1^18*t^2.97 + t^3. + t^3.68/g1^10 + t^4.01/g1^6 + (4*t^4.04)/g1^24 + g1^16*t^4.3 + t^4.34/g1^2 + (2*t^4.37)/g1^20 + g1^20*t^4.63 + (5*t^4.7)/g1^16 + 2*g1^6*t^4.99 + (4*t^5.02)/g1^12 + g1^10*t^5.32 + (4*t^5.35)/g1^8 + 2*g1^14*t^5.64 + t^5.67/g1^4 + t^5.71/g1^22 + g1^36*t^5.94 - 2*t^6. + (2*t^6.03)/g1^18 + (6*t^6.06)/g1^36 - g1^22*t^6.29 + (4*t^6.36)/g1^14 + (4*t^6.39)/g1^32 + 2*g1^8*t^6.65 + (3*t^6.68)/g1^10 + (10*t^6.72)/g1^28 + 2*g1^12*t^6.98 + (4*t^7.01)/g1^6 + (8*t^7.04)/g1^24 + g1^34*t^7.27 + g1^16*t^7.3 + (9*t^7.37)/g1^20 + g1^38*t^7.6 - g1^20*t^7.63 + 2*g1^2*t^7.66 + (6*t^7.7)/g1^16 + (2*t^7.73)/g1^34 + g1^6*t^7.99 + t^8.02/g1^12 + (3*t^8.05)/g1^30 + (9*t^8.09)/g1^48 - (2*t^8.35)/g1^8 + (6*t^8.38)/g1^26 + (6*t^8.41)/g1^44 + 2*g1^32*t^8.61 - 2*g1^14*t^8.64 - (4*t^8.67)/g1^4 + (6*t^8.71)/g1^22 + (16*t^8.74)/g1^40 + g1^54*t^8.9 + g1^36*t^8.94 - 4*g1^18*t^8.97 - t^4.34/(g1^2*y) - (2*t^6.36)/(g1^14*y) - t^6.68/(g1^10*y) - t^7.01/(g1^6*y) + t^7.04/(g1^24*y) + (2*t^7.37)/(g1^20*y) + (g1^2*t^7.66)/y + (4*t^7.7)/(g1^16*y) + (3*g1^6*t^7.99)/y + (4*t^8.02)/(g1^12*y) + (3*g1^10*t^8.32)/y + (2*t^8.35)/(g1^8*y) - (3*t^8.38)/(g1^26*y) + (2*g1^14*t^8.64)/y + (2*t^8.67)/(g1^4*y) + (g1^18*t^8.97)/y - (t^4.34*y)/g1^2 - (2*t^6.36*y)/g1^14 - (t^6.68*y)/g1^10 - (t^7.01*y)/g1^6 + (t^7.04*y)/g1^24 + (2*t^7.37*y)/g1^20 + g1^2*t^7.66*y + (4*t^7.7*y)/g1^16 + 3*g1^6*t^7.99*y + (4*t^8.02*y)/g1^12 + 3*g1^10*t^8.32*y + (2*t^8.35*y)/g1^8 - (3*t^8.38*y)/g1^26 + 2*g1^14*t^8.64*y + (2*t^8.67*y)/g1^4 + g1^18*t^8.97*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 |
|---|
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 |
|---|
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 560 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_2\phi_1^2$ + $ q_2^2\tilde{q}_1^2$ + $ M_2M_3$ + $ M_4\phi_1\tilde{q}_2^2$ | 0.7011 | 0.8806 | 0.7962 | [X:[], M:[0.6816, 1.1061, 0.8939, 0.6816], q:[0.7765, 0.5419], qb:[0.4581, 0.4358], phi:[0.4469]] | 2*t^2.04 + 2*t^2.68 + t^2.93 + t^3. + t^3.64 + t^3.7 + t^4.02 + 4*t^4.09 + t^4.27 + t^4.34 + t^4.59 + 4*t^4.73 + 2*t^4.98 + 2*t^5.04 + 3*t^5.36 + 2*t^5.61 + 3*t^5.68 + t^5.75 + t^5.87 - 2*t^6. - t^4.34/y - t^4.34*y | detail |