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 |
---|---|---|---|---|---|---|---|---|---|
58626 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1.3959 | 1.5865 | 0.8798 | [X:[1.3689], M:[0.7356], q:[0.3518, 0.6674], qb:[0.4904, 0.597], phi:[0.3156]] | [X:[[12]], M:[[-33]], q:[[25], [19]], qb:[[-22], [14]], phi:[[-6]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{6}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ | ${}$ | -1 | t^2.21 + t^2.53 + t^2.84 + t^2.85 + 2*t^3.47 + t^3.79 + t^4.11 + t^4.41 + 2*t^4.42 + t^4.73 + 2*t^4.74 + 2*t^5.05 + t^5.06 + 3*t^5.37 + 3*t^5.68 + 3*t^5.69 - t^6. + 3*t^6.01 + 3*t^6.31 + 2*t^6.32 + t^6.62 + 4*t^6.63 + t^6.64 + t^6.94 + 7*t^6.95 + 2*t^7.25 + 2*t^7.26 + 4*t^7.27 + 2*t^7.57 + 4*t^7.58 + 2*t^7.59 + 7*t^7.89 + 3*t^7.9 + t^7.91 + 8*t^8.21 + t^8.22 + 4*t^8.52 + 6*t^8.53 + t^8.54 + t^8.83 + 5*t^8.84 + 6*t^8.85 + t^8.84/y^2 - t^3.95/y - t^4.89/y - t^6.15/y - t^6.47/y - (2*t^6.79)/y - t^7.1/y - (2*t^7.42)/y - t^7.74/y + (2*t^8.05)/y - t^8.36/y + t^8.68/y - t^8.99/y - t^3.95*y - t^4.89*y - t^6.15*y - t^6.47*y - 2*t^6.79*y - t^7.1*y - 2*t^7.42*y - t^7.74*y + 2*t^8.05*y - t^8.36*y + t^8.68*y - t^8.99*y + t^8.84*y^2 | t^2.21/g1^33 + g1^3*t^2.53 + t^2.84/g1^18 + g1^39*t^2.85 + (2*t^3.47)/g1^3 + g1^33*t^3.79 + g1^12*t^4.11 + t^4.41/g1^66 + (2*t^4.42)/g1^9 + t^4.73/g1^30 + 2*g1^27*t^4.74 + t^5.05/g1^51 + g1^6*t^5.05 + g1^63*t^5.06 + (2*t^5.37)/g1^15 + g1^42*t^5.37 + (3*t^5.68)/g1^36 + 2*g1^21*t^5.69 + g1^78*t^5.69 - t^6. + 3*g1^57*t^6.01 + (3*t^6.31)/g1^21 + 2*g1^36*t^6.32 + t^6.62/g1^99 + (2*t^6.63)/g1^42 + 2*g1^15*t^6.63 + g1^72*t^6.64 + t^6.94/g1^63 + (4*t^6.95)/g1^6 + 3*g1^51*t^6.95 + (2*t^7.25)/g1^84 + (2*t^7.26)/g1^27 + 4*g1^30*t^7.27 + (2*t^7.57)/g1^48 + 4*g1^9*t^7.58 + 2*g1^66*t^7.59 + (2*t^7.89)/g1^69 + (5*t^7.89)/g1^12 + 3*g1^45*t^7.9 + g1^102*t^7.91 - t^8.21/g1^33 + 9*g1^24*t^8.21 + g1^81*t^8.22 + (4*t^8.52)/g1^54 + 6*g1^60*t^8.53 + g1^117*t^8.54 + t^8.83/g1^132 + (5*t^8.84)/g1^18 + 2*g1^39*t^8.85 + 4*g1^96*t^8.85 + t^8.84/(g1^18*y^2) - t^3.95/(g1^6*y) - t^4.89/(g1^12*y) - t^6.15/(g1^39*y) - t^6.47/(g1^3*y) - t^6.79/(g1^24*y) - (g1^33*t^6.79)/y - t^7.1/(g1^45*y) - (2*t^7.42)/(g1^9*y) - (g1^27*t^7.74)/y + t^8.05/(g1^51*y) + (g1^6*t^8.05)/y - t^8.36/(g1^72*y) - t^8.37/(g1^15*y) + (g1^42*t^8.37)/y + t^8.68/(g1^36*y) - t^8.99/(g1^57*y) - (t^3.95*y)/g1^6 - (t^4.89*y)/g1^12 - (t^6.15*y)/g1^39 - (t^6.47*y)/g1^3 - (t^6.79*y)/g1^24 - g1^33*t^6.79*y - (t^7.1*y)/g1^45 - (2*t^7.42*y)/g1^9 - g1^27*t^7.74*y + (t^8.05*y)/g1^51 + g1^6*t^8.05*y - (t^8.36*y)/g1^72 - (t^8.37*y)/g1^15 + g1^42*t^8.37*y + (t^8.68*y)/g1^36 - (t^8.99*y)/g1^57 + (t^8.84*y^2)/g1^18 |
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 |
---|---|---|---|---|---|---|---|---|---|
57731 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.4024 | 1.5963 | 0.8785 | [X:[1.3532], M:[0.7786], q:[0.3662, 0.6896], qb:[0.4721, 0.5317], phi:[0.3234]] | t^2.34 + t^2.51 + t^2.69 + t^2.91 + 2*t^3.49 + t^3.66 + t^4.06 + 2*t^4.46 + 2*t^4.63 + t^4.67 + t^4.85 + t^5.03 + t^5.21 + t^5.24 + t^5.25 + t^5.39 + t^5.4 + 2*t^5.43 + t^5.58 + 2*t^5.6 + 2*t^5.82 - 2*t^6. - t^3.97/y - t^4.94/y - t^3.97*y - t^4.94*y | detail |