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 |
|---|---|---|---|---|---|---|---|---|---|
| 45163 | SO5adj1nf2 | $M_1q_1q_2$ + $ M_2q_1^2$ + $ M_3\phi_1^2$ + $ M_4\phi_1^2q_1$ | 1.7858 | 1.8865 | 0.9466 | [X:[], M:[1.0547, 0.9994, 1.2968, 0.7965], q:[0.5003, 0.445], qb:[], phi:[0.3516]] | [X:[], M:[[-3, -3], [-6, 0], [2, 2], [-1, 2]], q:[[3, 0], [0, 3]], qb:[], phi:[[-1, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ q_2^2$, $ M_2$, $ M_1$, $ \phi_1^2q_2$, $ M_3$, $ \phi_1q_1q_2$, $ \phi_1^4$, $ M_4^2$, $ \phi_1^2q_2^2$, $ \phi_1^2q_1q_2$, $ M_4q_2^2$, $ \phi_1^2q_1^2$, $ q_2^4$, $ M_2M_4$, $ M_1M_4$, $ M_2q_2^2$, $ M_4\phi_1^2q_2$ | $M_2^2$, $ \phi_1^3q_1q_2$ | 0 | t^2.39 + t^2.67 + t^3. + t^3.16 + t^3.44 + 2*t^3.89 + t^4.22 + 2*t^4.78 + t^4.95 + t^5.06 + t^5.11 + t^5.34 + t^5.39 + t^5.55 + t^5.67 + t^5.83 + t^6.11 + t^6.16 - t^6.17 + 2*t^6.28 + t^6.33 + t^6.44 + 2*t^6.56 + t^6.61 - t^6.77 + 3*t^6.89 + t^7.05 + 2*t^7.17 + 3*t^7.33 + t^7.38 + 2*t^7.45 + t^7.5 + t^7.61 + t^7.66 + t^7.73 + 5*t^7.78 + 2*t^7.94 + t^8.01 + t^8.06 + 3*t^8.11 + 2*t^8.22 + t^8.34 + t^8.44 + t^8.5 + t^8.55 - t^8.56 + 3*t^8.67 + t^8.72 + t^8.78 + t^8.83 + 2*t^8.95 + t^8.99 - t^4.05/y - t^5.39/y - t^5.56/y - t^6.16/y - t^6.44/y - t^6.72/y - t^7.05/y - t^7.22/y - t^7.5/y - t^7.78/y - (2*t^7.95)/y - t^8.23/y - t^8.27/y - t^8.55/y + t^8.67/y - t^8.83/y - t^4.05*y - t^5.39*y - t^5.56*y - t^6.16*y - t^6.44*y - t^6.72*y - t^7.05*y - t^7.22*y - t^7.5*y - t^7.78*y - 2*t^7.95*y - t^8.23*y - t^8.27*y - t^8.55*y + t^8.67*y - t^8.83*y | (g2^2*t^2.39)/g1 + g2^6*t^2.67 + t^3./g1^6 + t^3.16/(g1^3*g2^3) + (g2*t^3.44)/g1^2 + 2*g1^2*g2^2*t^3.89 + t^4.22/(g1^4*g2^4) + (2*g2^4*t^4.78)/g1^2 + g1*g2*t^4.95 + (g2^8*t^5.06)/g1 + (g1^4*t^5.11)/g2^2 + g2^12*t^5.34 + (g2^2*t^5.39)/g1^7 + t^5.55/(g1^4*g2) + (g2^6*t^5.67)/g1^6 + (g2^3*t^5.83)/g1^3 - t^6. + t^6./g1^12 + (g2^7*t^6.11)/g1^2 + t^6.16/(g1^9*g2^3) - (g1^3*t^6.17)/g2^3 + 2*g1*g2^4*t^6.28 + t^6.33/(g1^6*g2^6) + (g2*t^6.44)/g1^8 + 2*g1^2*g2^8*t^6.56 + t^6.61/(g1^5*g2^2) - t^6.77/(g1^2*g2^5) + (3*g2^2*t^6.89)/g1^4 + t^7.05/(g1*g2) + (2*g2^6*t^7.17)/g1^3 + t^7.22/(g1^10*g2^4) - (g1^2*t^7.22)/g2^4 + 3*g2^3*t^7.33 + t^7.38/(g1^7*g2^7) + (2*g2^10*t^7.45)/g1^2 + g1^3*t^7.5 + g1*g2^7*t^7.61 + t^7.66/(g1^6*g2^3) + (g2^14*t^7.73)/g1 + (2*g2^4*t^7.78)/g1^8 + 3*g1^4*g2^4*t^7.78 + (2*g2*t^7.94)/g1^5 + g2^18*t^8.01 + (g2^8*t^8.06)/g1^7 + (3*t^8.11)/(g1^2*g2^2) + (2*g2^5*t^8.22)/g1^4 + (g2^12*t^8.34)/g1^6 + (g2^2*t^8.39)/g1^13 - (g2^2*t^8.39)/g1 + t^8.44/(g1^8*g2^8) + (g2^9*t^8.5)/g1^3 + t^8.55/(g1^10*g2) - (g1^2*t^8.56)/g2 + 2*g2^6*t^8.67 + (g2^6*t^8.67)/g1^12 + t^8.72/(g1^7*g2^4) + (g2^13*t^8.78)/g1^2 + (g2^3*t^8.83)/g1^9 + 2*g1*g2^10*t^8.95 + t^8.99/g1^18 - t^4.05/(g1*g2*y) - (g2^2*t^5.39)/(g1*y) - (g1^2*t^5.56)/(g2*y) - t^6.16/(g1^3*g2^3*y) - (g2*t^6.44)/(g1^2*y) - (g2^5*t^6.72)/(g1*y) - t^7.05/(g1^7*g2*y) - t^7.22/(g1^4*g2^4*y) - t^7.5/(g1^3*y) - (g2^4*t^7.78)/(g1^2*y) - (2*g1*g2*t^7.95)/y - (g1^2*g2^5*t^8.23)/y - t^8.27/(g1^5*g2^5*y) - t^8.55/(g1^4*g2*y) + (g2^6*t^8.67)/(g1^6*y) - (g2^3*t^8.83)/(g1^3*y) - (t^4.05*y)/(g1*g2) - (g2^2*t^5.39*y)/g1 - (g1^2*t^5.56*y)/g2 - (t^6.16*y)/(g1^3*g2^3) - (g2*t^6.44*y)/g1^2 - (g2^5*t^6.72*y)/g1 - (t^7.05*y)/(g1^7*g2) - (t^7.22*y)/(g1^4*g2^4) - (t^7.5*y)/g1^3 - (g2^4*t^7.78*y)/g1^2 - 2*g1*g2*t^7.95*y - g1^2*g2^5*t^8.23*y - (t^8.27*y)/(g1^5*g2^5) - (t^8.55*y)/(g1^4*g2) + (g2^6*t^8.67*y)/g1^6 - (g2^3*t^8.83*y)/g1^3 |
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 |
|---|---|---|---|---|---|---|---|---|
| 45283 | $M_1q_1q_2$ + $ M_2q_1^2$ + $ M_3\phi_1^2$ + $ M_4\phi_1^2q_1$ + $ M_5q_2^2$ | 1.7787 | 1.8721 | 0.9501 | [X:[], M:[1.0266, 1.0105, 1.3156, 0.8209, 1.0427], q:[0.4947, 0.4787], qb:[], phi:[0.3422]] | t^2.46 + t^3.03 + t^3.08 + t^3.13 + t^3.49 + 2*t^3.95 + t^4.11 + 2*t^4.93 + t^4.97 + t^5.02 + t^5.49 + t^5.54 + t^5.59 - t^6. - t^4.03/y - t^5.46/y - t^5.51/y - t^4.03*y - t^5.46*y - t^5.51*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 45064 | SO5adj1nf2 | $M_1q_1q_2$ + $ M_2q_1^2$ + $ M_3\phi_1^2$ | 1.7693 | 1.8564 | 0.9531 | [X:[], M:[1.0521, 1.0098, 1.2986], q:[0.4951, 0.4529], qb:[], phi:[0.3507]] | t^2.72 + t^3.03 + t^3.16 + t^3.46 + t^3.59 + 2*t^3.9 + t^4.21 + t^4.82 + t^4.95 + t^5.07 + t^5.43 + t^5.75 - t^6. - t^4.05/y - t^5.41/y - t^5.54/y - t^4.05*y - t^5.41*y - t^5.54*y | detail |