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 |
|---|---|---|---|---|---|---|---|---|---|
| 8912 | Sp2adj1nf1 | ${}\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}^{4}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}^{3}q_{1}^{2}$ + ${ }M_{5}\phi_{1}^{2}q_{1}q_{2}$ | 1.1553 | 1.3249 | 0.872 | [X:[1.5825], M:[1.1651, 1.0437, 0.8349, 0.7476, 0.8349], q:[0.3131, 0.4345], qb:[], phi:[0.2087]] | [X:[[4]], M:[[8], [-10], [-8], [12], [-8]], q:[[-3], [15]], qb:[], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }q_{1}q_{2}$, ${ }M_{3}$, ${ }M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}q_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }q_{1}^{2}q_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{4}\phi_{1}^{4}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{5}q_{1}q_{2}$, ${ }\phi_{1}^{4}q_{1}q_{2}$, ${ }X_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{3}\phi_{1}^{4}$, ${ }M_{5}\phi_{1}^{4}$, ${ }\phi_{1}^{8}$, ${ }M_{2}M_{4}$, ${ }M_{2}q_{1}q_{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{3}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{5}$, ${ }M_{2}\phi_{1}^{4}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{5}q_{2}^{2}$ | ${}$ | -2 | 2*t^2.24 + 3*t^2.5 + t^3.13 + t^3.23 + t^4.12 + 4*t^4.49 + 7*t^4.75 + 6*t^5.01 + 2*t^5.37 + 2*t^5.48 + 2*t^5.64 + 3*t^5.74 - 2*t^6. + 2*t^6.36 + t^6.47 + 2*t^6.63 + 6*t^6.73 - t^6.89 + 12*t^6.99 + 14*t^7.25 + t^7.35 + 9*t^7.51 + 2*t^7.62 + 4*t^7.72 + 4*t^7.88 + 6*t^7.98 + 3*t^8.14 - 6*t^8.5 + 4*t^8.61 + 2*t^8.71 - t^8.77 - t^8.87 + 12*t^8.97 + t^8.5/y^2 - (2*t^8.87)/y^2 - t^3.63/y - t^4.88/y - (2*t^5.87)/y - (3*t^6.13)/y - t^6.76/y - t^6.86/y - t^7.12/y - (2*t^7.38)/y + t^7.49/y + (6*t^7.75)/y + (2*t^8.01)/y - (4*t^8.11)/y - (3*t^8.37)/y + (2*t^8.48)/y - (2*t^8.64)/y + (3*t^8.74)/y - t^3.63*y - t^4.88*y - 2*t^5.87*y - 3*t^6.13*y - t^6.76*y - t^6.86*y - t^7.12*y - 2*t^7.38*y + t^7.49*y + 6*t^7.75*y + 2*t^8.01*y - 4*t^8.11*y - 3*t^8.37*y + 2*t^8.48*y - 2*t^8.64*y + 3*t^8.74*y + t^8.5*y^2 - 2*t^8.87*y^2 | 2*g1^12*t^2.24 + (3*t^2.5)/g1^8 + t^3.13/g1^10 + g1^28*t^3.23 + g1^6*t^4.12 + 4*g1^24*t^4.49 + 7*g1^4*t^4.75 + (6*t^5.01)/g1^16 + 2*g1^2*t^5.37 + 2*g1^40*t^5.48 + (2*t^5.64)/g1^18 + 3*g1^20*t^5.74 - 2*t^6. + 2*g1^18*t^6.36 + g1^56*t^6.47 + (2*t^6.63)/g1^2 + 6*g1^36*t^6.73 - t^6.89/g1^22 + 12*g1^16*t^6.99 + (14*t^7.25)/g1^4 + g1^34*t^7.35 + (9*t^7.51)/g1^24 + 2*g1^14*t^7.62 + 4*g1^52*t^7.72 + (4*t^7.88)/g1^6 + 6*g1^32*t^7.98 + (3*t^8.14)/g1^26 - (6*t^8.5)/g1^8 + 4*g1^30*t^8.61 + 2*g1^68*t^8.71 - t^8.77/g1^28 - g1^10*t^8.87 + 12*g1^48*t^8.97 + t^8.5/(g1^8*y^2) - (2*g1^10*t^8.87)/y^2 - t^3.63/(g1^2*y) - t^4.88/(g1^6*y) - (2*g1^10*t^5.87)/y - (3*t^6.13)/(g1^10*y) - t^6.76/(g1^12*y) - (g1^26*t^6.86)/y - (g1^6*t^7.12)/y - (2*t^7.38)/(g1^14*y) + (g1^24*t^7.49)/y + (6*g1^4*t^7.75)/y + (2*t^8.01)/(g1^16*y) - (4*g1^22*t^8.11)/y - (3*g1^2*t^8.37)/y + (2*g1^40*t^8.48)/y - (2*t^8.64)/(g1^18*y) + (3*g1^20*t^8.74)/y - (t^3.63*y)/g1^2 - (t^4.88*y)/g1^6 - 2*g1^10*t^5.87*y - (3*t^6.13*y)/g1^10 - (t^6.76*y)/g1^12 - g1^26*t^6.86*y - g1^6*t^7.12*y - (2*t^7.38*y)/g1^14 + g1^24*t^7.49*y + 6*g1^4*t^7.75*y + (2*t^8.01*y)/g1^16 - 4*g1^22*t^8.11*y - 3*g1^2*t^8.37*y + 2*g1^40*t^8.48*y - (2*t^8.64*y)/g1^18 + 3*g1^20*t^8.74*y + (t^8.5*y^2)/g1^8 - 2*g1^10*t^8.87*y^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 8823 | Sp2adj1nf1 | ${}\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}^{4}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}^{3}q_{1}^{2}$ | 1.1413 | 1.3017 | 0.8767 | [X:[1.5803], M:[1.1605, 1.0493, 0.8395, 0.7408], q:[0.3148, 0.426], qb:[], phi:[0.2099]] | 2*t^2.22 + 2*t^2.52 + t^3.15 + t^3.19 + t^3.48 + t^4.11 + 4*t^4.44 + 5*t^4.74 + 3*t^5.04 + 2*t^5.37 + 2*t^5.41 + t^5.67 + 4*t^5.7 - t^3.63/y - t^4.89/y - (2*t^5.85)/y - t^3.63*y - t^4.89*y - 2*t^5.85*y | detail |